Comparative heuristic analysis of pristine titanium, Ti6Al4V and Ti6Al7N powders.
\\n\\n
Released this past November, the list is based on data collected from the Web of Science and highlights some of the world’s most influential scientific minds by naming the researchers whose publications over the previous decade have included a high number of Highly Cited Papers placing them among the top 1% most-cited.
\\n\\nWe wish to congratulate all of the researchers named and especially our authors on this amazing accomplishment! We are happy and proud to share in their success!
Note: Edited in March 2021
\\n"}]',published:!0,mainMedia:{caption:"Highly Cited",originalUrl:"/media/original/117"}},components:[{type:"htmlEditorComponent",content:'IntechOpen is proud to announce that 191 of our authors have made the Clarivate™ Highly Cited Researchers List for 2020, ranking them among the top 1% most-cited.
\n\nThroughout the years, the list has named a total of 261 IntechOpen authors as Highly Cited. Of those researchers, 69 have been featured on the list multiple times.
\n\n\n\nReleased this past November, the list is based on data collected from the Web of Science and highlights some of the world’s most influential scientific minds by naming the researchers whose publications over the previous decade have included a high number of Highly Cited Papers placing them among the top 1% most-cited.
\n\nWe wish to congratulate all of the researchers named and especially our authors on this amazing accomplishment! We are happy and proud to share in their success!
Note: Edited in March 2021
\n'}],latestNews:[{slug:"intechopen-supports-asapbio-s-new-initiative-publish-your-reviews-20220729",title:"IntechOpen Supports ASAPbio’s New Initiative Publish Your Reviews"},{slug:"webinar-introduction-to-open-science-wednesday-18-may-1-pm-cest-20220518",title:"Webinar: Introduction to Open Science | Wednesday 18 May, 1 PM CEST"},{slug:"step-in-the-right-direction-intechopen-launches-a-portfolio-of-open-science-journals-20220414",title:"Step in the Right Direction: IntechOpen Launches a Portfolio of Open Science Journals"},{slug:"let-s-meet-at-london-book-fair-5-7-april-2022-olympia-london-20220321",title:"Let’s meet at London Book Fair, 5-7 April 2022, Olympia London"},{slug:"50-books-published-as-part-of-intechopen-and-knowledge-unlatched-ku-collaboration-20220316",title:"50 Books published as part of IntechOpen and Knowledge Unlatched (KU) Collaboration"},{slug:"intechopen-joins-the-united-nations-sustainable-development-goals-publishers-compact-20221702",title:"IntechOpen joins the United Nations Sustainable Development Goals Publishers Compact"},{slug:"intechopen-signs-exclusive-representation-agreement-with-lsr-libros-servicios-y-representaciones-s-a-de-c-v-20211123",title:"IntechOpen Signs Exclusive Representation Agreement with LSR Libros Servicios y Representaciones S.A. de C.V"},{slug:"intechopen-expands-partnership-with-research4life-20211110",title:"IntechOpen Expands Partnership with Research4Life"}]},book:{item:{type:"book",id:"8446",leadTitle:null,fullTitle:"Zinc Oxide Based Nano Materials and Devices",title:"Zinc Oxide Based Nano Materials and Devices",subtitle:null,reviewType:"peer-reviewed",abstract:"This book presents a review of recent advances in ZnO-based nanomaterials and devices. ZnO as a nanomaterial has gained substantial interest in the research area of wide bandgap semiconductors and is considered to be one of the major candidates for electronic and photonic applications. ZnO has distinguished and interesting electrical and optical properties and is considered to be a potential material in optoelectronic applications such as solar cells, surface acoustic wave devices, and UV emitters. ZnO's unique properties have attracted several researchers to study its electrical and optical properties. As a nanostructured material, ZnO exhibits many advantages for nanodevices. Moreover, it has the ability to absorb the UV radiation.",isbn:"978-1-78923-958-4",printIsbn:"978-1-78923-957-7",pdfIsbn:"978-1-78984-317-0",doi:"10.5772/intechopen.78819",price:119,priceEur:129,priceUsd:155,slug:"zinc-oxide-based-nano-materials-and-devices",numberOfPages:146,isOpenForSubmission:!1,isInWos:null,isInBkci:!1,hash:"7c1d14eb8eac769093f8d7a219a3884f",bookSignature:"Ahmed M. Nahhas",publishedDate:"October 9th 2019",coverURL:"https://cdn.intechopen.com/books/images_new/8446.jpg",numberOfDownloads:10460,numberOfWosCitations:12,numberOfCrossrefCitations:16,numberOfCrossrefCitationsByBook:1,numberOfDimensionsCitations:29,numberOfDimensionsCitationsByBook:1,hasAltmetrics:1,numberOfTotalCitations:57,isAvailableForWebshopOrdering:!0,dateEndFirstStepPublish:"September 6th 2018",dateEndSecondStepPublish:"November 5th 2018",dateEndThirdStepPublish:"January 4th 2019",dateEndFourthStepPublish:"March 25th 2019",dateEndFifthStepPublish:"May 24th 2019",currentStepOfPublishingProcess:5,indexedIn:"1,2,3,4,5,6,7",editedByType:"Edited by",kuFlag:!1,featuredMarkup:null,editors:[{id:"140058",title:"Prof.",name:"Ahmed",middleName:"M.",surname:"Nahhas",slug:"ahmed-nahhas",fullName:"Ahmed Nahhas",profilePictureURL:"https://mts.intechopen.com/storage/users/140058/images/system/140058.jpg",biography:"Ahmed M. Nahhas received his Master’s degree in Computer Engineering from Illinois Institute of Technology, Chicago, Illinois, USA in 1996 and a Ph.D. in Electrical Engineering (Electronics) from the University of Pittsburgh, Pittsburgh, Pennsylvania, USA in 2001. Professor Nahhas’s research has been centered on developing new photonic and electronic devices at micro and nano-scales involving various functional materials such as rare-earth-doped oxides, wideband gap semiconductors, and nanostructured materials. Prof. Nahhas’s research investigates epitaxial growth and fabrication of ZnO and GaN optical devices. Fabrication of MSM photo-detectors has been developed on a macro-scale area of wafer surface using a directed self-organization method and has been investigated as an interaction medium in optical, electrical, chemical, and biological domains. Surface-Plasmon phenomena occurring in structures are of particular interest since many novel properties can be derived from those and can be incorporated into an on-chip configuration for interaction. Professor Nahhas has participated in reviewing several academic articles and dissertations in the area of electrical, electronics, communications, control engineering, and e-learning. He is an official reviewer of journals such as the American Journal of Nanomaterials—USA, many International conferences, and holds the Associate Professor position at several Saudi Universities. Professor Nahhas served in many prestigious leading positions including Dean of the College of Engineering at Al-Lith, head of the Department, Vice Dean at Umm Al Qura University, Makkah. Currently, he works at the College of Engineering and Islamic Architecture, Umm Al Qura University, Makkah, Kingdom of\nSaudi Arabia.",institutionString:"Umm al-Qura University",position:null,outsideEditionCount:0,totalCites:0,totalAuthoredChapters:"2",totalChapterViews:"0",totalEditedBooks:"1",institution:{name:"Umm al-Qura University",institutionURL:null,country:{name:"Saudi Arabia"}}}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,coeditorOne:null,coeditorTwo:null,coeditorThree:null,coeditorFour:null,coeditorFive:null,topics:[{id:"208",title:"Material Science",slug:"nanotechnology-and-nanomaterials-material-science"}],chapters:[{id:"66694",title:"Introductory Chapter: Overview of ZnO Based Nano Materials and Devices",doi:"10.5772/intechopen.85969",slug:"introductory-chapter-overview-of-zno-based-nano-materials-and-devices",totalDownloads:863,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:null,signatures:"Ahmed M. Nahhas",downloadPdfUrl:"/chapter/pdf-download/66694",previewPdfUrl:"/chapter/pdf-preview/66694",authors:[{id:"140058",title:"Prof.",name:"Ahmed",surname:"Nahhas",slug:"ahmed-nahhas",fullName:"Ahmed Nahhas"}],corrections:null},{id:"64716",title:"Structural and Luminescence Properties of ZnO Nanoparticles Synthesized by Mixture of Fuel Approach in Solution Combustion Method",doi:"10.5772/intechopen.82467",slug:"structural-and-luminescence-properties-of-zno-nanoparticles-synthesized-by-mixture-of-fuel-approach-",totalDownloads:1180,totalCrossrefCites:2,totalDimensionsCites:3,hasAltmetrics:0,abstract:"Zinc oxide has been used for many applications, for example optoelectronic devices, ceramics, catalysts, pigments, varistors and many other important applications. In this study, ZnO nanoparticles were synthesized by mixture of fuel approach in solution combustion method. Mixtures of urea, glycine and citric acid were mixed at room temperature with Zinc nitrates as fuels resulting in spontaneous ignition resulting in production of ZnO nanopowder. The crystal structure and size of the synthesized powder were determined by X-ray diffractometer (XRD), which revealed that the synthesized ZnO nanopowder has the pure wurtzite structure having crystallite size 26–40 nm. Optical studies of nanomaterial were examined by FTIR and UV-Visible absorption spectrum. The luminescence studies also investigated in the visible region 360–800 nm with excitation 325 nm laser. These nanomaterials may be used in solid-state lightening devices.",signatures:"Trilok K. Pathak and H.C. Swart",downloadPdfUrl:"/chapter/pdf-download/64716",previewPdfUrl:"/chapter/pdf-preview/64716",authors:[{id:"242320",title:"Dr.",name:"Trilok Kumar",surname:"Pathak",slug:"trilok-kumar-pathak",fullName:"Trilok Kumar Pathak"}],corrections:null},{id:"65533",title:"Green Synthesis of Zinc Oxide Nanostructures",doi:"10.5772/intechopen.83338",slug:"green-synthesis-of-zinc-oxide-nanostructures",totalDownloads:3865,totalCrossrefCites:8,totalDimensionsCites:13,hasAltmetrics:0,abstract:"ZnO-based nanomaterials have been proven to be of great use for several leading applications since the beginning of nanoscience due to the abundance of zinc element and the relatively easy conversion of its oxide to nanostructures. Nowadays, ZnO as nanoparticles, nanowires, nanofibers as well as plenty of other sophisticated nanostructures takes place among the pioneer nanomaterials employed in the photovoltaic systems, fuel cells, and biomedical fields. Nevertheless, optimizing energy consumption and being eco-friendly are the challenging requirements that are still to be overcome for their synthesis. Green chemistry has been strongly presented recently in the scientific arena as an adequate potential alternative; worldwide investigations have been held on subjects involving bacteria, fungus, or algae-based synthesis as efficient options, and some of the intriguing scientific findings on this subject are reported hereafter.",signatures:"Tuğba Isık, Mohamed Elhousseini Hilal and Nesrin Horzum",downloadPdfUrl:"/chapter/pdf-download/65533",previewPdfUrl:"/chapter/pdf-preview/65533",authors:[{id:"262515",title:"Dr.",name:"Nesrin",surname:"Horzum",slug:"nesrin-horzum",fullName:"Nesrin Horzum"},{id:"278120",title:"Mr.",name:"Mohamed",surname:"Elhousseini Hilal",slug:"mohamed-elhousseini-hilal",fullName:"Mohamed Elhousseini Hilal"},{id:"278122",title:"Ms.",name:"Tuğba",surname:"Isık",slug:"tugba-isik",fullName:"Tuğba Isık"}],corrections:null},{id:"68125",title:"Doped Zinc Oxide Nanostructures for Photovoltaic Solar Cells Application",doi:"10.5772/intechopen.86254",slug:"doped-zinc-oxide-nanostructures-for-photovoltaic-solar-cells-application",totalDownloads:1383,totalCrossrefCites:3,totalDimensionsCites:5,hasAltmetrics:0,abstract:"Zinc oxide and doping effects of Cu on its structural, morphological, optical, and surface wettability properties and the consequent influence on photoelectrochemical solar cell performance has been reviewed. Cu dopant in the doping solution is varied in the range of 1 to 5 at.% which significantly affected the properties of ZnO. Slight changes in the lattice parameters of the Cu-doped zinc oxide (CZO) electrodes were reported, due to the successful substitution of Zn2+ by Cu2+ and also enhancement in crystallinity of the films at 3 at.% Cu due to reduction in crystallographic defects in the film. Surface morphologies were reported with densely grown nanorods over the varied range of Cu, with 3 at.% having the densest microstructures with average diameter approximately 125 nm. A review of optical properties indicated significant enhancement in absorption edge of approximately 60 nm into the visible band for the nanorods with 3 at.% Cu content due to light scattering. Optical energy band-gaps decrease from 3.03 to 2.70 eV with Cu doping. Surface wettability was adjudged hydrophilic for all the films, implying high porosity and water contact angles depended on Cu content. Photoelectrochemical cell performance indicated an n-type photoactivity in sodium sulfate (Na2SO4) electrolyte, which motivates to check its feasibility in solar cell applications.",signatures:"Tyona MD",downloadPdfUrl:"/chapter/pdf-download/68125",previewPdfUrl:"/chapter/pdf-preview/68125",authors:[{id:"277047",title:"Dr.",name:"Mrumun David",surname:"Tyona",slug:"mrumun-david-tyona",fullName:"Mrumun David Tyona"}],corrections:null},{id:"64820",title:"Pyrolysis of Carbon-Doped ZnO Nanoparticles for Solar Cell Application",doi:"10.5772/intechopen.82098",slug:"pyrolysis-of-carbon-doped-zno-nanoparticles-for-solar-cell-application",totalDownloads:959,totalCrossrefCites:1,totalDimensionsCites:2,hasAltmetrics:0,abstract:"It is very important to find new methods for improving the properties of nanostructured materials that can be used to replace the highly expensive and complicated techniques of fabricating ZnO nano-powders for solar cell applications. Pneumatic spray pyrolysis method offers a relatively inexpensive way of fabricating ZnO nanomaterials of controllable morphology, good crystallinity and uniform size distribution, which makes it a good candidate for the production of ZnO nanoparticles. Additionally, it has the advantage of producing ZnO NPs in one step directly on the substrate without the need for other wet chemistry processes like purification, drying and calcination. To that end, the present study emphasizes more on the design and optimization of spray pyrolysis system as well as on the pneumatic spray pyrolysis conditions for the production of carbon-doped ZnO nanoparticles. The un-doped and carbon-doped ZnO NPs were prepared using pneumatic spray pyrolysis employing zinc acetate as a precursor solution and tetrabutylammonium as a dopant. The fabricated un-doped and C-ZnO NPs were characterized for their morphological, structural and optical properties using SEMEDX, XRD and DRS. SEM analysis has revealed that the fabricated un-doped and C-ZnO NPs have spherical shape with mesoporous morphology. The cross-sectional SEM has also revealed that the film thickness changes with increasing dopant concentration from 0.31 to 0.41 μm at higher concentrations. Moreover, the EDX spectra have confirmed the presence of Zn and O atoms in the PSP-synthesized ZnO NPs. XRD analysis of both un-doped and C-ZnO has revealed the peaks belonging to hexagonal Wurtzite structure of ZnO. Additionally, the DRS has revealed a decrease in energy band gap of the synthesized ZnO NPs, with the increase in carbon dopant level.",signatures:"Luyolo Ntozakhe and Raymond Tichaona Taziwa",downloadPdfUrl:"/chapter/pdf-download/64820",previewPdfUrl:"/chapter/pdf-preview/64820",authors:[{id:"196100",title:"Dr.",name:"Raymond",surname:"Taziwa",slug:"raymond-taziwa",fullName:"Raymond Taziwa"},{id:"278261",title:"Mr.",name:"Luyolo",surname:"Ntozakhe",slug:"luyolo-ntozakhe",fullName:"Luyolo Ntozakhe"}],corrections:null},{id:"65480",title:"Surface-Enhanced Raman Spectroscopy (SERS) Based on ZnO Nanorods for Biological Applications",doi:"10.5772/intechopen.84265",slug:"surface-enhanced-raman-spectroscopy-sers-based-on-zno-nanorods-for-biological-applications",totalDownloads:1043,totalCrossrefCites:2,totalDimensionsCites:4,hasAltmetrics:1,abstract:"Detection of nanometer-sized biomarkers is a research topic that attracts much attention as an application for early diagnosis of diseases. Biopsy monitoring by analyzing cell secretion in a non-destructive way has many advantages in the field of biomedicine. We introduce the Raman signal enhancement method on a biosensing chip based on surface-enhanced Raman diagnosis. This approach has the advantage because the ZnO nanorods are grown to form nanoscale porosity and are coated with gold to enable size selective biomarker detection. After sputtering gold on the grown ZnO nanostructures, the unique feature of clustering the nanorod’s heads first appeared. The grain formation on the head was the main factor for the localized surface plasmon resonance (LSPR) enhancement, and this fact could be verified by finite element analysis. It has been demonstrated in breast cancer cell line that the cell viability is also high in such gold-clad ZnO nanostructure-based surface-enhanced substrates. For bioapplication, interstitial cystitis/bladder pain syndrome (IC/BPS) animal model was prepared by injecting HCl into the bladder of a rat, and urine was collected a week later to conduct Raman spectroscopy experiments.",signatures:"Sanghwa Lee and Jun Ki Kim",downloadPdfUrl:"/chapter/pdf-download/65480",previewPdfUrl:"/chapter/pdf-preview/65480",authors:[{id:"7162",title:"Prof.",name:"Jun Ki",surname:"Kim",slug:"jun-ki-kim",fullName:"Jun Ki Kim"},{id:"280897",title:"Dr.",name:"Sanghwa",surname:"Lee",slug:"sanghwa-lee",fullName:"Sanghwa Lee"}],corrections:null},{id:"67613",title:"Anodic ZnO-Graphene Composite Materials in Lithium Batteries",doi:"10.5772/intechopen.86169",slug:"anodic-zno-graphene-composite-materials-in-lithium-batteries",totalDownloads:1168,totalCrossrefCites:0,totalDimensionsCites:2,hasAltmetrics:0,abstract:"An important area to cope with in the implementation of technologies for the generation of energy from renewable sources is storage, so it is a priority to develop new ways of storing energy with high efficiency and storage capacity. Experimental reports focused on ZnO-graphene composite materials applied to the anode design which indicated that they show low efficiencies of around 50 %, but values very close to the theoretical capacity have already been reported in recent years. The low efficiency of the materials for the anode design of the Li-ion battery is mainly attributed to the pulverization and fragmentation of the material or materials, caused by the volumetric changes and stability problems during the charge/discharge cycles. In this chapter, we will discuss the development of composite materials such as ZnO-graphene in its application for the design of the anode in the Li-ion battery.",signatures:"Herrera-Pérez Gabriel, Pérez-Zúñiga Germán, Verde-Gómez Ysmael, Valenzuela-Muñiz Ana María and Vargas-Bernal Rafael",downloadPdfUrl:"/chapter/pdf-download/67613",previewPdfUrl:"/chapter/pdf-preview/67613",authors:[{id:"152334",title:"Dr.",name:"Gabriel",surname:"Herrera-Pérez",slug:"gabriel-herrera-perez",fullName:"Gabriel Herrera-Pérez"},{id:"182114",title:"D.Sc.",name:"Rafael",surname:"Vargas-Bernal",slug:"rafael-vargas-bernal",fullName:"Rafael Vargas-Bernal"},{id:"300122",title:"MSc.",name:"Germán",surname:"Pérez-Zúñiga",slug:"german-perez-zuniga",fullName:"Germán Pérez-Zúñiga"},{id:"301446",title:"Dr.",name:"Ana Maria",surname:"Valenzuela-Muñiz",slug:"ana-maria-valenzuela-muniz",fullName:"Ana Maria Valenzuela-Muñiz"},{id:"301447",title:"Dr.",name:"Ysmael",surname:"Verde-Gómez",slug:"ysmael-verde-gomez",fullName:"Ysmael Verde-Gómez"}],corrections:null}],productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"},subseries:null,tags:null},relatedBooks:[{type:"book",id:"7640",title:"Perspective of Carbon Nanotubes",subtitle:null,isOpenForSubmission:!1,hash:"8b85a9957fad5206369eadf0c1ffa27d",slug:"perspective-of-carbon-nanotubes",bookSignature:"Hosam El-Din Saleh and Said Moawad Mohamed El-Sheikh",coverURL:"https://cdn.intechopen.com/books/images_new/7640.jpg",editedByType:"Edited by",editors:[{id:"144691",title:"Prof.",name:"Hosam M.",surname:"Saleh",slug:"hosam-m.-saleh",fullName:"Hosam M. 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D in Physics in 2012 from Indian Institute of Technology Guwahati, India. Presently, he is associated with the Faculty of Science, Sri Sri University, India as an Assistant Professor in Physics. Prior to joining the current\naffiliation, he was a postdoctoral fellow at different renowned institutions, Kobe University Japan, S. N. Bose National Centre for Basic Sciences, India and Cardiff University, United Kingdom. He was awarded prestigious JSPS postdoctoral fellowship based on his research contribution on semiconducting nanowires. He has published more than 32 research articles including 1 review article in high profile international journals and 3 book chapters to his credit. 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Subsequently, he joined the Department of Botany, Sikkim University,\nIndia, as an assistant professor. He has published more than 100 articles in peer-reviewed journals and books. He has edited and written several books and contributed chapters on different aspects of plant sciences including light sources generally\nused in controlled agriculture, genetic transformation, and secondary metabolites\nof medicinal plants. 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One of the most significant and costly problems of modern medicine is the necessity to replace or supplement organs or tissues to prevent the biological and social degradation of patients and to restore their living functions, either normal functions or such acceptably similar to normal, resulting from a growing number of cases of organ or tissue loss or damage in the human population due to post-injury or post-resection losses as well as those originating from the operative treatment of cancerous tumours or inflammation processes and as a result of other disorders, and also work, traffic and sports accidents. The most widespread cases are caused by a strong development of civilisational diseases, including cancer, and the incidence rate of malignant cancers has been regularly rising. The number of traffic accident victims has been growing substantially, as well [2]. One of the fundamental tasks globally is to improve the society\'s condition of health, medical care and health safety. The idea is to overcome problems which occur more and more often and to protect against serious health risks, especially such as civilisational diseases, pandemics and bioterrorism and to support research, particularly research into the development of modern technologies, serving to advance medicine and healthcare, most of all to replace the lost tissues and organs by technical means, to ensure more complete prophylactics of diseases and safe treatment of patients, which are one of the important indicators of economic welfare. Bone reconstruction, for example, of legs and hands and in the craniofacial area, as well as skin and other soft tissue reconstruction, and also the reconstruction of oesophagus and blood vessels, are often required due to the consequences of civilisational diseases and accidents, including malignant cancers. Patients\' healthcare expectations are also growing, and economic aspects at the global scale call for the efficient elimination of disabilities, in particular motoric disabilities, and the restoration of the previously handicapped persons to physical fitness and usually most often to full, or at least partial, professional activity, which considerably lessens pressure on the diminishing resources of social insurance funds. It is vital to reduce waiting times for treatment, to lower prices and to improve availability of medical products or services and therapy, to reduce the risk of treatment failure, in particular by tailor-made personalised medical products according to a patient\'s individual anatomical features, and ultimately to reduce therapy discomfort for patients and their family.
The development of regenerative medicine started nearly a quarter of century ago along with the works [3], consisting of treatment by replacing old and sick cells with young cells using tissue engineering methods and cell-based therapies or gene therapy and creating numerous new opportunities in counteracting diseases and their consequences [4–8]. On the other hand, tissue engineering – introduced somewhat earlier [9] – consists of the development of biological substitutes for restoration, maintenance or improvement of functions of tissues or entire organs [10, 11], involving the construction and fabrication of scaffolds maintaining the developing tissues and involving the production of a replacement tissue for clinical use [12] as a substitute of damaged tissues or entire organs [13, 14], capable of restoring, maintaining or improving the functions of particular tissues or organs [10]. It is obviously a continued endeavour to develop an engineering material with its properties corresponding to the tool being replaced, supplemented or aided, which does not cause an immunological response of the immunity system and expediting wound healing and not causing implant rejection. The advancement of tissue engineering methods poses further challenges for biomaterials which should not only be fully compatible, but when used for three-dimensional scaffolds, should ensure conditions for cellular cultures, taking into account the possibility of controlled growth, division and differentiation of different types of cells and the impact of various environmental factors on their living functions, and also for transporting medicines in a patient\'s organism.
Among the biocompatible materials currently and widely used in many branches of industry are titanium and its alloys. These materials are characterised by excellent corrosion resistance in the majority of aggressive environments. Titanium has two allotrope types: Tiα and Tiβ. The α allotrope type endures to the temperature of 882°C and crystallises in a hexagonal structure with a compact lattice (A3). The β allotrope type endures to the temperature of 882–1068°C being a melting point and it crystallises in a regular structure with a centred spatial lattice (A2) [15]. Titanium alloys are classified as single-phase α and β, double-phase α + β and pseudo-α and pseudo-β. Double-phase α + β alloys are the most popular, widely used group of titanium alloys with good strength and plastic properties. This group includes the most popular Ti6Al4V titanium alloy. Titanium and titanium alloys, conventionally manufactured by casting and plastic treatment [16], are used in the arms, chemical, automotive, aviation, power and transport sector, as well as in architecture and sports [17–20]. Pristine titanium and its alloys, independent of the wide engineering application, are often used in medicine in order to replace damaged tissues. From many years, these materials have been used for endoprosthesis of hip-joints and knee-joints, bone plates, screws for fracture repair and heart valve prostheses [21–24]. Moreover, artificial heart is currently developed using these materials [25]. Recently, for medical applications, materials sintered from powders of pristine titanium, Ti6Al4V and Ti6Al7Nb are also applied [21–25]. Table 1 shows comparative analysis of these materials.
No. | Evaluation criteria | Ti | Ti6Al4V | Ti6Al7Nb |
---|---|---|---|---|
1 | The current use of this material in medicine | High | Very high | Minor |
2 | Powder granulation, μm | 10–45 | 15–45 | 0–100 |
3 | Density, g/cm3 | 4.51 | 4.43 | 4.52 |
4 | Melting point, °C | 1600–1660 | 1660 | 1520–1580 |
5 | Price, €/kg (state for 2014 year) | 400 | 500 | 250 |
6 | Availability | High | High | Low |
7 | Powder application in SLS/SLM process | Yes | Yes | No |
Comparative heuristic analysis of pristine titanium, Ti6Al4V and Ti6Al7N powders.
A structure of the extracellular matrix (ECM) occurring in living organisms, and acting as a natural scaffold of cells [26], can be imitated by biomaterials which, for this reason, can find their application as a substrate for the controlled breeding of living cells. Capable of growth, division and differentiation are such living cells only, which are attached to a substrate and have undergone adsorption on a substrate surface. In natural conditions, this is possible owing to the presence of the extracellular matrix. The coincidence of a metallic substrate with living cells is a very vital aspect. It is also vital to determine the potential favourable effect of indirect layers – in the form of thin coatings deposited onto the inner surfaces of pores of a metallic skeleton made of titanium and its alloys produced by SLS – on the potential adhesion and proliferation of living cells. Not all the factors are known, which are decisive for the influence of a substrate made of engineering materials on the attachment, division and growth of living cells, despite the fact that intensive research has been conducted in this field. A material\'s specificity is one of the most essential factors crucial for the breeding or growth of cells on the surface of engineering materials [27, 28]. The domains ensuring the adhesion of cells to a substrate are very important in interactions between living organisms and engineering materials in cultures of living stem cells and in implantology. The one which is best recognised is arginyl glycyl aspartic acid (RGD), which is a tripeptide composed of l-arginine, glycine, and l-aspartic acid, as well as other proteins, including integrins, cadherins, selectins and immunoglobulin-like proteins [29–37]. After placing an implant in an organism, its surface is covered with a thin layer of water within a few seconds, and then, within a few seconds to several hours, with a layer of specific proteins [38] from those contained in physiological fluids [39]. A weakly vascularised, fibrous layer of cells [29, 40] is growing on such cells within several minutes to several days, and finally a cytoskeleton of cells is reorganised, leading notably to the flattening of cells [41]. Surface wettability influences the ability of adhesion proteins to attach to the substrate, and their affinity to the material surface has influence on the structure and composition of a layer of proteins [38]. The free enthalpy of surface and its wettability influence the growth of cells, but do not have an effect on their shape and orientation [42–44]. The adhesion domains placed on the surface of engineering biomaterials influence the behaviour of cells due to an effect on the functioning of integrins [29]. Cells\' material attachability depends on proteins\' substrate adhesion [29–35, 37–39, 42, 45]. An excessively hydrophilic and hydrophobic character of the surface with the wetting angle of over 80 or below 15° [46] is sometimes unfavourable for the growth of cells, although surface hydrophobicity may, in the initial phase, support cells\' adhesion, when hydrophilicity may support their division and multiplication [47]. In general, cells are preferentially attaching, dividing and growing on hydrophilic surfaces of a material, whilst their ability of adhesion to a substrate material is diminishing on hydrophobic surfaces [38, 39, 47–53].
As flexibility of different types of cells varies [54–66], their morphology and living functions depend on the stiffness of the substrate on which they are grown [54–69]. Usually cells\' differentiation ability increases due to increased material stiffness, although exceptions to this rule exist [55, 57, 58, 60–66]. Because cells are interacting with the substrate surface [55, 57, 58, 60–66, 70], the cells growing on a stiff substrate exhibit greater rigidity [64, 67, 71], a more organised cellular cytoskeleton [55, 59, 63–67] and greater flattening [55, 57, 60, 63–66, 70, 72] than those growing on a more elastic substrate. Cells, especially fibroblasts and cells of smooth muscles, exhibit mechanotaxis (durotaxis), moving towards a substrate with greater rigidity [57, 62, 64–66, 72, 73]. Increased substrate rigidity is decisive for the reduced ability of cells to migrate [65], and different types of cells react differently to differentiated rigidity of a substrate made of engineering materials [54]. A material\'s surface topography influences cells\' adhesion ability [74, 75], and they show an ability of adaptation to a material\'s surface specificity [53, 76–79]. Surface topography is dictating proteins\' adhesion and creation of bonds, which is essential for material biocompatibility, influencing also morphology, spatial orientation, division and differentiation of cells [38, 80]. Cells\' behaviour is also influenced by surface texture and smoothness [2, 38, 74, 76, 77, 81–84]. Cell adhesion is more difficult on less developed surfaces with higher smoothness [85], whereas the division of osteoblasts is faster on surfaces with smaller smoothness [86–88], opposite to fibroblasts which are proliferating fastest on smoother surfaces [56, 89–92]. The flattening of cells is decreasing as the smoothness of the substrate surface is deteriorating [86, 88, 91, 92].
Additive technologies [93–95] can be employed, in particular, for producing different implants, including dental implants and bridges, individualised implants of the upper jaw bone, hip joint and skull fragments using suitable biomaterials. An exceptional usefulness of additive technologies of producing solid and microporous materials in medicine and dentistry has been confirmed by comparing powder metallurgy technologies, casting technologies, metallic foam manufacturing technologies and additive manufacturing technologies with procedural benchmarking techniques [96, 97] using a universal scale of relative states for comparative evaluation [96–99]. Considering the additive technologies applied most widely in industry, only few have found their application in prosthetics, especially in prosthodontics, that is, electron beam melting (EBM) [100–105], and also 3D printing for production of indirect models, although selective laser sintering/selective laser melting offers broadest opportunities (SLS/SLM) [100, 106–125]. The sintering/melting of grains takes place by remelting the particles of a new powder on the surface with the existing piece of an item being constituted by a laser beam moving in a programmed fashion in line with the pre-defined geometrical characteristics of a metal element being produced. SLS/SLM technologies are so attractive due to the opportunities offered by 3D design with the use of CAD methods and due to the related overall control over the materials fabricated, both, in terms of the structure, sizes and repeatability of geometric features. Microskeletons with controlled sizes and shapes of pores can also be manufactured.
A microporous element manufactured by SLS can be further worked and combined with other materials, for example, by infiltration or internal treatment of pores\' surface in an appropriately chosen technological process [117–121, 126–128]. Titanium and titanium alloys from Al, Nb and Ta [1, 2, 15, 26, 127–138], well tolerated by a human organism, have been long used in medicine and dentistry for prosthetic and implantological purposes, also fabricated by SLS. Titanium matrix materials do not cause allergic reactions and are stainless, feature high strength and hardness and also thermal conductivity several times lower than traditional prosthetic materials [139]. Titanium is a very thrombogenic material [140], and biocompatibility, especially thrombocompatibility [141] of this material can be enhanced by introducing alloy elements. Pores are dimensionally adapted to be filled by the reconstructed cells and their migration and also neovascularisation [142] for preventing blood clots [143]. Their section cannot be too small to prevent their sealing [144]. A porous structure of scaffolds should secure the diffusion of nutrients and metabolism products. Permanently fixated scaffolds do not ensure scaffold removal as is the case with scaffolds removable during regeneration in the natural condition [143–145]. Other metallic materials can also be utilised for this purpose, for example, polymer materials [40, 81, 146–153] or polymer matrix composite materials with a fraction of metals or ceramic particles [81, 150]. Unlike metals and their alloys, polymer materials can be not only biocompatible, but also biodegradable and bioresorbable [29, 46, 154, 155], and also in some cases osteoinductive [156] and can reduce thrombogenic properties of the material [40]. Another concept relates, however, to covering the surface of metallic materials with other materials, also as a result of working an internal surface of pores [125, 157]. Porous metallic materials, chiefly Ti and Ta [158] and Mg [159], are used for non-biodegradable scaffolds primarily due to relatively high compressive strength and fatigue strength [160, 161]. Coatings of internal surfaces of pores are used, however, because they meet the imposed requirements better than metals and their alloys [40, 162, 163]. The following is necessary, especially, not to cause disease-related changes: the lack of a toxic effect of the implant material, the lack of its mutagenic properties, the lack of its effect on the composition of body fluids, both by the material being implanted as well as in the case of polymer materials, also by its decomposition products [40, 81, 147].
Original own works [117–120, 126, 164–180] have been undertaken concerning constructional solutions and fabrication technologies of a new generation of custom, original, hybrid, microporous high-strength engineering and biological materials with microporous rigid titanium and titanium alloy skeletons manufactured by selective laser sintering, whose pores are filled with living cells (Figure 1). This will ensure the natural ingrowth of a living tissue, at least in the connection zone of prosthetic/implant elements, with bone or organ stumps, and will eliminate the need to apply for patients the mechanical elements which are positioning and fixating the implants. The so constructed and fabricated implants, in the connection zone with bone stumps, contain a porous zone, with surface treatment inside pores, enabling the living tissues to grow and they remain in an organism permanently and do not require re-operation.
Chart of constructional assumptions (a) hybrid and multilayer biologically active microporous composite engineering materials consisting of biologically active cellular structures and of implant-scaffolds; (b) implant-scaffolds with microporous zones acting as scaffolds.
As the adhesion and growth of living cells are dependent on the type and characteristics of the substrate, in order to implement the planned concept of manufacturing engineering and biological materials and implant-scaffolds, it is required to seek the most advantageous proliferation conditions of living cells inside the pores of a microporous skeleton made of titanium and titanium alloys, which is the underlying scope of the research presented in this chapter. It appears that the improvement of proliferation conditions of cells is ensured by a substrate made of fully compatible materials, including TiO2, Al2O3 oxides and a hydroxyapatite, Ca10(PO4)6(OH)2. For this reason, it was decided to employ these materials as coatings of internal surfaces of pores of a microporous skeleton fabricated by SLS. Two technologies have been chosen, respectively, for the deposition of thin coatings onto the internal surfaces of pores, ensuring the uniform thickness of coatings on all the walls and openings of a substrate being coated, even with highly complicated shapes, that is, the so-called atomic layer deposition (ALD) [96, 124, 126, 128, 181–184] (Figure 2) and the sol-gel technology of coating deposition from the liquid phase by the immersion method [96, 181, 185–194] (Figure 3).
Sequence of the phenomena associated with ALD technology [
Sequence of the phenomena associated with the sol-gel technology of coating deposition [
The elements used for the research were produced by an additive method by powder sintering in an SLS process. Selective laser sintering can be grouped into a stage of designing a given element, the outcome of which is a 3D CAD model in the .
Selective laser sintering technology process diagram [
The following was used for model designing: Solid Works 2015 Pro and 3D Marcarm Engineering AutoFab (Software for Manufacturing Applications) software, version Autofab MCS 2.0 and Autofab MTT 64 and the CAD/CAM tools available in, respectively, SLM 250H system by MTT Technologies Group and in AM 125 system by Renishaw for selective laser sintering. The software enables to select model dimensions, constructional features, the type of the model volume filling either as solid or porous and to choose the size of a cell unit making up the entire model. A set of “hexagon cross” unit cells was used, selected in a geometrical analysis, and as a result of preliminary studies, from the set available in the software. By duplicating them, the entire elements were designed, consisting of nodes and single lattice fibres, linking the particular skeleton node (Figure 5). Fabrication conditions were also selected, at the stage of virtual design of elements, achievable in, respectively, SLM 250H system by MTT Technologies Group and AM 125 by Renishaw for selective laser sintering, including layer thickness, laser power, laser beam diameter, scanning rate, distance between particular remelting paths. A spatial orientation of unit cells of 45° relative to the
(a, b) Hexagon cross unit cell; (c) image of structure of computer models presenting the arrangement of unit cells in the space of the system of coordinates at the angle of 45° relative to the
It was very important to establish the correct laser power value, ranging between 50 and 200 W, and the laser beam diameter, of 30–150 μm, and also the distance between laser beams and distance between laser remelting paths equal to or smaller than the laser beam diameter in case of solid elements, as opposite to the variant when it is larger than the laser beam diameter, which is decisive for the porosity of the produced element. Such conditions were selected as a result of preliminary studies.
When a model is designed and the selected fabrication conditions are taken into account, it is transferred to the software of the SLM 250H system machine by MTT Technologies Group or AM 125 by Renishaw, where selective laser sintering takes place. The YFL fibre laser, with an active material doped with Ytterbium and the maximum power of, respectively, 400 and 200 W, was used in the devices. The skeleton microporous materials, fabricated by SLS, exhibit porosity which depends on the manufacturing conditions, including mainly laser power and laser beam diameter and the distance between laser beams and the distance between laser remelting paths. Solid titanium with the density of 4.51 g/cm3, corresponding to the density of solid titanium given in literature, can be achieved if the laser power of 110 W is applied. The smallest porosity of 61–67% corresponds to the selectively laser sintered elements with the highest mass and the average pore size of ~250 μm, whereas the highest porosity of 75–80% corresponds to elements with the smallest mass and the average pore size of ~450 μm. The porosity of 70–75% was obtained for the average pore size of ~350 μm.
Two types of powders with a spherical shape were used, respectively, for selective laser sintering to produce solid specimens and microporous skeletons (Figure 6a, b) and with the composition shown in Table 2, also confirmed with spectral examinations with the energy dispersive spectrometry (EDS) method (Figure 6c, d):
titanium powder with Grade 4 and grain size of up to 45 μm, oxygen concentration reduced to 0.14%, the aim of which is to ensure process safety,
Ti6Al4V alloy powder with the grain diameter of 15–45 μm, for medical applications.
Powder of (a) Ti, (b) Ti6Al4V alloy (SEM), (c, d) relevant diagrams of EDS [
Ti | 0.01 | 0.03 | 0.14 | 0.01 | 0.004 | <0.4 | <0.01 | Remainder | ||
Ti6Al4V | 6.35 | 4.0 | 0.01 | 0.2 | 0.15 | 0.02 | 0.003 | ≤0.4 | ≤0.1 |
Chemical composition of the powders used for selective laser sintering.
Figure 7a and b and shows a surface structure of pristine titanium and Ti6Al4V alloy manufactured by selective laser sintering with laser beam size of 50 μm and laser power of 110 W. Chemical composition, examined with an EDS spectrometer, shows that Ti only exists in the first case in the sample (Figure 7c), and Ti, Al and V (Figure 7d) were identified in the other case, which corresponds to the data given in Table 2 for chemical composition of powders used for selective laser sintering. It was revealed in both cases that, apart from the completely sintered materials with revealed paths of laser beam transition, fine powder particles exist, as well, which – after sintering – should be removed mechanically or by chemical etching. On the surface of porous titanium microskeletons (Figures 8–10), apart from sintered titanium, there are grains of powder loosely bonded with a skeleton, which were not fully melted with a titanium microskeleton; the results of local remelting also exist, as indicated by the surface topography of porous titanium skeletons for the different arrangement of cell units. In order to remove such unfavourable surface effects, porous titanium, after selective laser sintering, was subjected to preliminary cleaning in an isopropyl alcohol solution with an ultrasound washer. After getting rid of excessive powder from the pores of the titanium skeleton, it was subjected to etching in an aqua regia solution with the fraction volume of 3:1 HCl:HNO3, for 1 hour with an ultrasound washer, to etch the surface remelting not removed in preliminary cleaning and the fine powder particles not attached permanently to the previously constituted titanium microskeleton. The samples were subjected to etching in an aqua regia solution, as a result of which about 3% of the sintered material mass was removed (Figure 11). The roughness of skeletons before etching is much higher than after etching
Surface structure of solid samples manufactured by selective laser sintering with the use of laser beam of 50 μm with laser power of 110 W; SEM of (a) solid titanium, (b) Ti6Al4V alloy, (c, d) respectively, EDS charts [
Titanium scaffold (a) visible with bare eye, (b, c) stereoscope microscope, (d–f) SEM.
Surface typography of porous titanium skeletons with different pore size: (a) 350 μm, (b) 450 μm, (c) 630 μm; SEM.
Surface topography of microskeletons made of Ti6Al4V alloy manufactured as multiplication of different unit cells presented with different magnificence (a, b, c); SEM images.
Surface topography of porous titanium skeletons with the pore size of ~450 μm (a) after etching in aqua regia solution (SEM), (b) after ultrasound cleaning, (c) after etching in aqua regia solution; (b, c) laser confocal microscope.
The structural examinations of selectively laser sintered titanium and Ti6Al4V alloy were carried out in a transmission electron microscope, TITAN 80–300, by FEI. Titanium and Ti6Al4V alloy have a crystalline structure, hence for the appropriately high microscope resolution, one can observe the rows of atoms arranged parallel to each other, both, when the microscope is in the TEM transmission mode and in the STEM scanning-transmission mode (Figure 12).
Crystalline structure of: (a) pristine titanium, (b) Ti6Al4V alloy; HRTEM image.
It is not possible to use standard normalised conditions of mechanical tests due to a porous structure of the analysed materials, which are not covered by the system of EN standards, and also due to the manufacturing costs and time of the samples for tests of mechanical properties and due to a limited size of a working chamber and manufacturing device efficiency. A custom, own method was therefore established for performing such examinations with a universal tensile testing machine, Zwick 020, in the conditions principally corresponding to static tensile tests, three-point bending and compression tests. Moreover, specially adapted miniaturised samples were also produced for examinations of strength properties (Figure 13), with the dimensions of measuring parts of, respectively, 3 × 3 × 15 mm, 3 × 10 × 35 mm (for support spacing of 30 mm) and 10 × 10 × 10 mm.
Image of computer model of solid samples for static test: (a) tensile test, (b) three-point bending test, (c) compression test.
The mechanical properties of solid and porous materials fabricated by SLS, that is, sintered titanium and sintered Ti6Al4V alloy, were compared each time. The results of examinations of, respectively, tensile strength, bending strength and comprehensive strength were presented in such order. The impact of laser power ranging 70–110 W was investigated in the first place on tensile strength values of sintered titanium and sintered Ti6Al4V alloy. The results of examinations for five samples, for each treatment option of each of such materials, are presented in Figure 14.
Comparison of diagrams of dependency between tensile stress and elongation for solid samples made of Ti6Al4V alloy and pristine titanium sintered at different laser powers [
Figure 15 presents the comparison of diagrams of dependency between tensile stress and elongation for solid and porous laser sintered Ti and Ti6Al4V alloy samples with the pore size of approx. 250 μm, subjected to static tensile tests. The results were obtained to compare the conditions of selective laser sintering, that is, with the laser power of 60 W, which is favourable for porous materials. The examinations pinpoint, however, they are completely unacceptable for solid materials.
Comparison of diagrams of dependency between tensile stress and elongation for solid and porous laser sintered Ti and Ti6Al4V alloy samples with the pore size of approx. 250 μm [
Bending strength tests were performed the same as tensile strength tests. The geometrical characteristics of the samples given in Figure 13 were selected. The tests were carried out in relation to the investigated solid materials, that is, sintered titanium, sintered Ti6Al4V alloy as well as in relation to porous materials manufactured by SLS. The results concerning such tests were obtained as previously, for comparable conditions of selective laser sintering, that is, for the laser power of 60 W. The impact of laser power ranging 70–110 W on bending strength values of sintered titanium and sintered Ti6Al4V alloy for five samples for each treatment variant of each of the materials is shown in Figure 16. Figure 17 compares the diagrams of dependency between bending stress and deflection for solid and porous Ti and Ti6Al4V alloy samples with the pore size of approx. 250 μm, selectively laser sintered in the given conditions.
Comparison of diagrams of dependency between bending stress and deflection for solid samples made of Ti6Al4V alloy and pristine titanium sintered at different laser powers [
Comparison of diagrams of dependency between bending stress and deflection for solid and porous selectively laser sintered Ti and Ti6Al4V alloy samples with the pore size of approx. 250 μm [
The results of compressive strength tests are also presented for solid and porous Ti and Ti6Al4V alloy samples with the pore size of approx. 250 μm, selectively laser sintered with the laser power of 60 W (Figure 18).
Comparison of diagrams of dependency between compressive stress and deformation for solid and porous selectively laser sintered Ti and Ti6Al4V alloy samples [
The ALD technique enables to deposit a chosen TiO2 coating very uniformly across the entire surface of a part being treated, also if this part has a porous structure, as is the case with scaffolds. Changes in the sample colour, depending on the number of the executed ALD cycles, hence depending on the thickness of the deposited TiO2 layer, is an interesting phenomenon observed with a bare eye (Figure 19) and in a light stereoscopic microscope, Discovery V12 Zeiss, allowing to view colourful magnified images. An uncoated element has silver-metallic colour, and when subjected to surface treatment by the ALD method, it becomes, respectively: brown-gold (500 cycles), navy blue (1000 cycles) and light blue with silver shade (1500 cycles) (Figure 19).
Titanium scaffolds coated with TiO2 layers deposited by ALD; (a–c) cubic scaffolds viewed with bare eye, (d–f) stereoscopic scaffold images made with the magnification of 32× after: (a, d) 500 cycles, (b, e) 1000 cycles, (c, f) 1500 cycles.
Scaffolds manufactured by the selective laser sintering method from powders of titanium and biocompatible Ti6Al4V titanium alloy, then coated with a thin layer of Al2O3 in the process of deposition of single atomic layers, ALD, were examined – analogously as TiO2 layers – by means of a stereomicroscope, Discovery V12 Zeiss, allowing to identify that – along with the changing deposition thickness of an ALD layer – the colour of scaffolds is changing. The scaffolds, onto which Al2O3 layers were deposited in 500 cycles, are dark brown; such onto which Al2O3 layers were deposited in 1000 cycles are navy blue, and such onto which Al2O3 layers were deposited in 1500 cycles are dark blue (Figure 20). The differences in colours are also visible with a bare eye.
Surface topography of scaffolds manufactured from: (a–c) pristine titanium; (d–f) Ti6Al4V alloy; and coated with a layer of Al2O3 in: (a, d) 500; (b, e) 1000; (c, f) 1500 cycles; stereoscope microscope.
The measurements of layers\' thickness with a spectroscope ellipsometer for each sample with deposited TiO2 layers were performed in 25 places and statistical calculations were carried out, which has permitted to create a series of 2D maps of thickness distribution of the deposited atomic layers (Figure 21). The average thickness of TiO2 layers deposited by ALD technique for the analysed cases of 500, 1000 and 1500 cycles is, respectively, 56, 99 and 149 nm. The difference in the thickness of the deposited TiO2 layers on the studied area does not exceed 2 nm, which can be analysed in detail by studying layer thickness distribution maps. The best results were obtained for a layer deposited in 1000 cycles. A difference in the thickness of the deposited layer in this case does not exceed 1.1 nm across the entire area of the surface-treated item.
Titanium scaffolds coated with TiO2 layers deposited by ALD after: (a, b) 500 cycles, (c, d) 1000 cycles, (e, f) 1500 cycles; (a, c, e) thickness deposition maps; (b, d, f) AFM image of 3D surface topography.
The topography of the scaffolds\' surface coated with TiO2 layers, deposited by the ALD method, was examined by means of an atomic force microscope, AFM XE-100 Park System, in two and three dimensions (Figure 22). There are irregularities with a nanometric scale on the scaffold surface, the number of which is rising proportionally to the number of the deposited layers. In particular, a layer deposited in 500 cycles has a rather uniform granular structure and the larger clusters of atoms are occurring on it only occasionally. In the case of a layer deposited in 1000 cycles, clusters of atoms with a diameter of about 1 μm occur every several microns. The biggest clusters of atoms, forming “islands” with the length of up to several micrometres, occur in the case of a layer deposited in 1500 cycles.
Scaffold surface with TiO2 layer deposited in 1500 cycles presented with different magnificence (a, b, c); SEM images.
The detailed surface morphology examinations of the produced TiO2 layers were performed with an electron scanning microscope, Supra 35, by Zeiss, with the accelerating voltage of 10–20 kV (Figure 22). Secondary Electrons detection with SE detectors by In Lens was used to obtain surface topography images. A nanometric thickness of TiO2 layers deposited by ALD results in the fact that the layers can be observed in a scanning electron microscope only for very high magnifications of 150kx (Figure 22). A clear difference between a scaffold surface without surface treatment and scaffold surface covered with a TiO2 layer in an ALD process can be observed only when such high magnifications are used. The scaffold surface, immediately following fabrication, is smooth with clear longitudinal bands arranged every several dozen/several hundreds of nanometres, corresponding to the laser activity direction. The deposited atomic TiO2 layer, when magnified by approx. 150kx, is visible as a “sheep”, that is, a set of numerous adjacent oval granules of which only a few have a larger diameter.
The detailed surface morphology examinations of thin Al2O3 layers produced in a process of deposition of single atomic ALD layers, the same as TiO2 layers, was examined by means of a scanning electron microscope, Supra 35, by Zeiss, with the accelerating voltage of 2–10 kV (Figures 23 and 24) with different magnification of up to 100kx inclusive. The examinations performed with the highest magnification allow to spot a clear difference between the scaffold surface without surface treatment and the scaffold surface with a deposited layer of aluminium oxide, which is coated with convexities with the size of up to approx. 10 nm if 500 cycles are used, to approx. 200 nm if layers are deposited in 1500 cycles (Figures 23 and 24).
Surface topography of scaffolds manufactured from: (a–c) pristine titanium; (d–f) Ti6Al4V alloy and coated with Al2O3 layer in: (a, d) 500; (b, e) 1000; (c, f) 1500 cycles; SEM.
High-resolution surface topography of scaffolds manufactured from: (a–c) pristine titanium; (d–f) Ti6Al4V alloy and coated with Al2O3 layer in: (a, d) 500; (b, e) 1000; (c, f) 1500 cycles; SEM.
A TiO2 layer deposited by ALD onto a surface of a scaffold made of pristine titanium is of an amorphous structure, opposite to a crystalline titanium structure clearly shown in TEM images (Figure 25), as confirmed by TiO2 layer examinations with a transmission electron microscope, TITAN 80–300 by FEI. Depending on the number of cycles, the thickness of a TiO2 layer deposited by ALD varies between several dozens to hundred and a few dozens of nanometres. The examinations of TiO2 layers with a transmission electron microscope on samples in a form of thin foils prepared with a focused ion beam microscope (FIB) with the use of gallium arsenide with deposition of a thin layer of platinum show that the both chemical elements, apart from titanium and oxygen, are found on the EDS chart from an area situated on the periphery of the deposited layer, located in the direct neighbourhood of the protected layer of platinum (Figure 25). The EDS examinations of the deposited layers carried out in the region closer to the substrate reveal the presence of titanium and oxygen only (Figure 25), as is also confirmed by a prepared distribution map of chemical elements (Figure 26).
Amorphous TiO2 layer deposited onto pristine titanium with a crystalline structure in a technological process lasting 1500 cycles; (a–c) HRTEM; (d, e) qualitative analysis of EDS chemical composition of TiO2 layer: (d) from the peripheral region contiguous to the protective platinum layer; (c) near a titanium substrate.
Distribution map of chemical elements present in the TiO2 layer situated near titanium substrate.
In order to confirm the presence of layers consisting of TiO2 on the surface of a scaffold fabricated from TiAl6V4 powder, qualitative examinations of chemical composition were performed with the EDS scattered X-ray radiation spectroscopy method using an EDS (energy dispersive spectrometer), and a scaffold not containing a TiO2 layer was considered a reference material. An analysis of the diagrams shown in Figure 27 indicates that a spectrum was recorded in both cases with reflexes distinctive for titanium, aluminium and vanadium, whereas a reflex coming from titanium and oxygen exists additionally in a material covered with a layer of ALD, which corresponds to the occurrence of a TiO2 layer on the surface of this material. Examinations were also undertaken using the inVia Reflex device by Renishaw, being an automated Raman system. A Raman spectrum obtained with the wave dispersion method, after base line correction, within the spectral range of 150–3200 cm−1, is coming from a material being a scaffold, while a Raman spectrum coming from a material coated with a thin layer of titanium dioxide is shown in Figure 27, which – just like an EDS analysis – confirms the presence of titanium, aluminium and vanadium in the reference material; moreover oxygen, present in the surface layer, is found – apart from such chemical elements – in a material coated with a TiO2 layer.
(a) Qualitative analysis of EDS chemical composition of TiO2 layer; (b, c) results of qualitative analysis of chemical composition of: (b) TiAl6V4 without ALD layer, (c) TiAl6V4 with TiO2 layer deposited by ALD method after 1500 cycles; (d) Raman spectrum of Ti6Al4V scaffold deposited by ALD method with TiO2 layer [
It was found, with special WiRETM 3.1 software, that a layer deposited by the ALD method is anatase, being a polymorphous type of titanium dioxide. Figure 28 shows the images of points where spectra were recorded, originating from a reference Ti6Al4V scaffold and a scaffold covered with a layer of TiO2; the images were made with a confocal microscope being a constituent part of the inVia Reflex device.
Points where Raman spectra were recorded, originating from: (a) reference Ti6Al4V scaffold, (b) Ti6Al4V scaffold covered with a layer of TiO2; images coming from a confocal microscope.
Structural examinations were performed with the X-ray diffraction (XRD) method (Figure 29) with an X´Pert Pro X-ray diffractometer by Panalytical (CuKα radiation, λ = 1.54050∙10−10 m) using filtered radiation of a copper lamp with the voltage of 45 kV and a filament current of 35 mA, and the deposited TiO2 layers were examined with the razing-incidence method due to the small thickness of not more than 150 nm, thus extinguishing the peaks coming from the substrate. Reflexes coming from three polymorphous variants of titanium dioxide, that is, anatase, rutile and brookite, were identified in the examinations.
X-ray diffraction pattern of TiO2 layer applied by atomic layer deposition (ALD) performed with the razing-incidence X-ray diffraction method.
In order to confirm that the observed ALD layers are fabricated from Al2O3 aluminium oxide, qualitative examinations were performed of chemical composition with the EDS scattered X-ray radiation spectroscopy method and were displayed as diagrams in Figure 30. For thin Al2O3 layers, deposited on a scaffold made of titanium, spectra were recorded with reflexes characteristic for aluminium and oxygen, coming from a layer and for titanium coming from the substrate (Figure 30a). A spectrum was recorded for a Ti6Al4V scaffold, with reflexes characteristic for titanium and vanadium, coming from the substrate and oxygen from the layer. The reflex recorded from aluminium comes from the coating and substrate (Figure 30b). Distribution maps of chemical elements were additionally performed in the investigated materials. The presence of titanium, aluminium and oxygen was found in a titanium scaffold coated with aluminium oxide, and additionally vanadium is also found in a scaffold produced from Ti6Al4V. Supplementary X-ray examinations were also performed as a result of which no crystalline phase of aluminium oxide was found for ALD layers, which indicates their amorphous form. Such a result is expected due to the analogy with TiO2 layers – deposited with the same method – subjected to examinations at a nanometric scale. An amorphous structure of the deposited layers is clearly seen in TEM images as opposed to crystalline titanium being the substrate.
EDS spectrum made for scaffolds manufactured from: (a) pristine titanium; (b) Ti6Al4V titanium alloy; and coated with Al2O3 layers in 500 cycles.
Thin layers of hydroxyapatite were deposited with the immersion sol-gel technique (dip coating). The solution was prepared using hydroxyapatite nanopowder (HA), polyethylene glycol (PEG), glycerine and ethyl alcohol. The scaffolds manufactured from pristine titanium and Ti6Al4V alloy, coated with a layer of hydroxyapatite, manufactured by the sol-gel technique, were examined by means of a stereomicroscope microscope, Discovery V12 ZEISS. The detailed surface morphology examinations of the produced layers were undertaken with an electron scanning microscope Supra 35 by Zeiss. SEM images of thin layers were presented, on which hydroxyapatite particles are visible (Figures 31 and 32). The shape of the majority of hydroxyapatite particles is oval, however, a large content of particles with an elongated shape, with rounded, sometimes sharpened edges, is observed. The size of hydroxyapatite particles can be estimated at 20–80 nm. In case of sol-gel layers deposited on a scaffold made of titanium, spectra were recorded with reflexes characteristic for calcium, phosphorus and oxygen coming from a layer, and being the main hydroxyapatite components, and a reflex for titanium coming from the substrate (Figure 33). Similarly, for a scaffold made of Ti6Al4V alloy, spectra were recorded with reflexes characteristic for calcium, phosphorus and oxygen coming from the layer, and titanium, aluminium and vanadium, coming from the substrate. In addition, distribution maps of chemical elements were additionally performed in the investigated samples. Titanium was identified in a pure Ti scaffold, and also vanadium if Ti6Al4V alloy was also used. In the samples covered with a sol-gel layer, apart from the chemical elements coming from the substrate (e.g. titanium or titanium, aluminium and vanadium), calcium, phosphorus and oxygen were additionally identified, coming from a layer of hydroxyapatite (Figure 33). Structural examinations of sol-gel layers were performed by means of an X-ray structure analysis. Reflexes were identified coming from hydroxyapatite (Figure 34).
Scaffold made of Ti with the sol-gel layer of hydroxyapatite deposited after 10 immersions presented with different magnificence (a, b); SEM images.
Scaffold made of Ti6Al4V alloy with the sol-gel layer of hydroxyapatite deposited after 10 immersions presented with different magnificence (a, b); SEM images.
EDS spectrum of scaffold made of: (a) Ti, (b) Ti6Al4V: With a sol-gel layer of hydroxyapatite deposited after 10 immersions.
X-ray diffraction pattern of hydroxyapatite layer made with the sol-gel method.
One of the many elements largely influencing the quality of the society\'s life is the standard of healthcare. For this reason, all the activities in this sphere are considered as priorities in social policy in many countries and by international organisations. The life quality of patients after mechanical injuries, with tumorous and genetic diseases and with lost teeth greatly depends on the technical level, innovativeness and avant-garde solutions for medical and dental implants. It is obvious that the successfulness of the medical care provided depends on competencies of the doctors performing diagnostics, taking relevant decisions, applying appropriate therapies and related surgical procedures. The issue is a synergy of the actions jointly undertaken by medical doctors and engineers. The aspects of engineering-assisted medicine relate, both, to the constructional, material and technological design of, in particular, medical and dental implants. The development of medical implants is largely dependent upon advancements in biomaterials engineering, characterised by the required biological compatibility and harmonious interaction with living matter, without acute or chronic reactions, nor an inflammatory condition of the surrounding tissues after introduction into an organism. The advanced research efforts described in this chapter concern the engineering aspects of development of innovative implant-scaffolds, which enable the adhesion and proliferation of a patient\'s living cells into an intentionally designed porous structure of an implant which, on one hand, acts as an element transferring high stresses existing in an organism, and on the other hand acts as a scaffold into which a patient\'s cells are growing into. Metallic materials, despite their disadvantages, such as insufficient corrosive resistance and insufficient biotolerance in some areas of applications, are characterised by a pool of very advantageous mechanical properties. High fatigue corrosion resistance, brittle cracking resistance and tensile and bending strength should be considered especially significant. However, weak susceptibility of metallic materials as a substrate for cells\' development is undoubtedly an issue. An effect of a substrate on the proliferation of living cells has been described in detail based on comprehensive literature studies. This aspect is very complex. Porous metallic materials are an attractive implantation material due to better, as compared to traditional alloys, accommodation of the elasticity modulus to the bone and because bone tissue can grow on pores and by ensuring appropriate implant fixation to the bone. Dedicated technologies ensuring surface treatment inside pores with the size of 200–400 μm are fully innovative and require very advanced nanotechnological instrumentation. Titanium and titanium alloys belong to a group of metallic materials applied for many years in the fabrication of implants for bone surgery, maxillo-facial surgery and prosthodontics. The principal reasons include relatively low density, a beneficial strength-to-yield stress limit ratio, good corrosive resistance and best biocompatibility in this group of biomaterials. Titanium and titanium alloys are considered as such allowing to eliminate the risk associated with a harmful effect of chemical elements occurring as alloy additives in metallic materials, and concerns and controversies around some of them have not been scientifically proven until now.
A porous scaffold, with its dimensions and shape perfectly suited to a patient\'s tissue loss, made of a biocompatible material (Ti or Ti6AlV4), additionally coated with a nanometric layer of osteoconductive titanium oxide, aluminium oxide or hydroxyapatite inside pores, seems to be a breakthrough solution. It is a highly hybridised and composite engineering material, fabricated by a hybrid technology combining avant-garde and experimental additive technologies of selective laser sintering SLS, in conjunction with ALD and sol-gel technologies appropriate for nanotechnology. Modern CAD/CAMD software allows to convert the data acquired at a clinical stage into a 3D solid model of a patient\'s lost tissues. The model is then converted into a porous model through the multiplication of a unit cell whose dimensions and shape may be designed according to a patient\'s individual preferences. The pores existing in the material structure have the diameter of up to 500 μm and should be open, because a scaffold, in its intended conditions of use, is to grow through a patient\'s living tissue.
This chapter presents the outcomes of numerous author\'s complementary technological, structural and strength investigations which are a basis for optimised selection of engineering materials, adequate technologies and constructional assumptions for completely new and innovative products. Biomimetic, light, porous, rough and biocompatible materials with unique mechanical and functional properties finding their application for completely innovative scaffolds and implant-scaffolds can be manufactured owing to a custom combination of advanced methods of computer aided materials design and selective laser sintering (SLS) of titanium and Ti6AlV4 alloy powders with avant-garde deposition methods of single atomic ALD or sol-gel methods. A series of the investigations performed to date, in which technological conditions were established for the fabrication of this type of coatings inside pores, was completed successfully, which is presented thoroughly in this chapter. The role of the manufactured layers, with their thickness which can be programmed in advance, and not only controlled
Since the ultrafast (femtosecond) laser was demonstrated in the 1980s, the field of terahertz (THz) technologies has emerged with an array of applications appearing in different areas, from spectroscopy and sensing to imaging and high-speed communications [1, 2]. Terahertz radiation is nonionizing radiation and has low photon energies, thus having less chance of tissues, cells, and DNA damage during the spectroscopic, sensing, and imaging applications. In addition, the terahertz radiation can be transmitted through some opaque objects in visible light, which opens an array of detection and security applications. The late development of the THz applications is due to the challenges in the generation and detection within the THz band. Its frequencies of 0.1 to 10 THz (30 μm to 3 mm), sandwiched between the electronic and optical frequencies, cannot be generated by conventional electronics or optical methods [3]. This is because the conventional electronics technologies are insufficient to produce broadband waves at these relatively high frequencies. On the other hand, conventional optical technologies cannot emit THz frequencies due to a fundamental issue; there is no material with a bandgap energy corresponding to the THz frequencies [4]. Fortunately, various ultrafast laser and semiconductors approaches have been examined and established. That leads to demonstration of the first emission of pulsed THz radiation using a dipole photoconductive antenna in 1988 by Smith
The photoconductive THz emitter is an optoelectronic device with three main components, being the photoconductive materials, the photoconductive electrodes, and the lens [8] (Figure 1). The photoconductive material is a semiconductor having bandgap energy compatible with the photon energy of the ultrashort laser pulses. In addition, the photoconductive material should have optimum characteristics, including carrier lifetime, carrier mobility, breakdown voltage, and dark resistivity [9]. The carrier lifetime is preferable to be short. However, in the case of the photoconductive detector, it must be in the subpicosecond range. A higher breakdown voltage, carrier mobility, and dark resistivity are fundamental characteristics to assure a better photoconductive THz emitter performance in the form of higher radiated power, higher SNR, and broader bandwidth. The second component is the photoconductive electrodes. The photoconductive electrodes are two metal electrodes patterned on top of the device, having a gap in between, namely, a photoconductive gap. The design and dimensions of such a gap will influence the device’s performance. The last component is the lens. The lens is typically integrated with the emitter to accumulate the radiated field; the radiated field will then be focused on the targeted radiation path.
Illustration of the photoconductive device, as in (a) it shows a schematic diagram of the photoconductive THz emitter, and in (b) it shows the semiconductor band structure under the applied electric field. © IOP publishing. Reproduced with permission. All rights reserved [
The photoconductive THz emitter can generate the THz radiation following photoexcitation of its photoconductive gap by an ultrashort laser pulse. When the laser pulse is focused into a photoconductive gap, the laser pulse generates free electrons and holes within the semiconductor, having a rate proportional to the laser pulse [10]. The free carriers will then accelerate under a bias field, controlled by the bias voltage,
This chapter presents the photoconductive devices for THz generation, with insights into their components, limitations, and considerations, and recent progress in this field. In Section 2, a number of photoconductive materials are discussed, the influence of the material and material’s characteristics are addressed. In Section 3, the photoconductive electrodes (structure) are considered. This includes different structures characteristics based on their size, being a large aperture antenna, a small aperture antenna, and the plasmonic antenna, discussing the influences on the photoconductive THz emitters’ performance. In Section 4, the limitations of the THz emission by photoconductive devices are discussed. The presented limitations are mainly related to the bias field and optical (pump) fluence, which appear in the form of radiated power saturation. In addition, the underlying physics of the space charge and near-field saturation is provided. Ultimately, in Section 5, the recent advances in photoconductive devices technology are given, including the integrated devices and the system-on-chip technologies.
In general, the photoconductive THz emitter performance differs based on the photoconductive material and structure. Therefore, the photoconductive material will be the focus of this section. The optimum photoconductive materials would be crystal lattices with a direct bandgap between the valence and conduction bands. This bandgap determined the absorption wavelength of the exciting laser pulse. Other factors that play a significant role in choosing suitable materials are low carrier lifetime and high carrier mobilities. The most studied materials for photoconductive devices are gallium arsenide (GaAs), indium gallium arsenide (InGaAs), quantum well of InGaAs, indium aluminum arsenide (InAlAs), and a combination of group III-VI materials. This section will explore the photoconductive materials GaAs, ion-implantation in GaAs, InGaAs, and multi-quantum wells InGaAs/InAlAs.
Gallium Arsenide (GaAs) is a III–V semiconductor that has a bandgap of (Eg ∼ 1.42 eV at 300 K) corresponding to the emission wavelength of 880 nm [12]. GaAs is compatible with the titanium-doped sapphire (Ti: sapphire) femtosecond pulsed laser sources typically used to illuminate the photoconductive THz emitters. The GaAs has been the most common material and is typically employed in semi-insulating (SI)-GaAs, low temperature-grown (LT)-GaAs, or ion-implanted GaAs. The SI-GaAs grown by liquid-encapsulated Czochralski at 450–600°C [13] is typically a single crystal that has a high resistivity (>107 Ω cm) and a high electron mobility (μ > 7000 cm2/Vs) [14]. The SI-GaAs is considered a cost-effective substrate and has become widely used material for photoconductive devices. However, the research was ongoing to shorten the carrier lifetime. The LT-GaAs grown on SI-GaAs is proved to reduce carrier lifetime two orders of magnitude to below 1 ps compared to SI-GaAs (t > 100 ps) and efficiently generate broadband THz radiations of over 1 THz with high resistivity (107 Ω cm) and reasonable mobility μ (100–300 cm2/Vs) [15]. The growth is typically done by molecular beam epitaxy (MBE) on the surface of SI-GaAs substrate and growth temperature to between 200°C and 300°C in an arsenic-rich environment [16]. In such a case, it yields a high level of crystallinity, which means higher carrier mobilities and point defects due to excess As precipitants. Higher mobility leads to fast response, and point defects significantly reduce the lifetime (below 400 fs). These point defects act as recombination centers [15]. Increasing the temperature above 250°C will increase the lifetime to be greater than 50 ps. Tani
An alternative approach is using the ion-implantation technique to create point defects and reduce the lifetime in SI-GaAs by implementing arsenic, oxygen, nitrogen, carbon, and hydrogen (proton). Implanting H+ ions are shown to decrease the carrier lifetime of GaAs to sub-picosecond. Then several groups studied the effect of As+3 ion implantation of SI-GaAs and introduced excess As+3 impurities within the crystal structure similar to LT-GaAs [11]. However, the ion-implantation technique of As+3 (GaAs∶ As+3) improved the controllability of the excess As+3 concentration and uniformity as compared to LT-GaAs, making it more reproducible than LT growth [11]. Salem
The InGaAs are also employed as photoconductive material. It is a great advantage of the III-V compound to engineer the bandgap by changing the composition ratio. For example, the bandgap of the ternary compound indium gallium arsenide (InxGax-1As) can be potentially varied from 1.42 eV (x = 0) to 0.36 eV (x = 1). From a practical point of view, the protentional to achieve 0.8 eV (1550 nm optical excitation) was the motivation for investigating this material for THz applications. Doping InGaAs by iron has been demonstrated to provide required recombination sites for a subpicosecond carrier lifetime, higher optical pump saturation power, and higher breakdown voltage. Wood
Heterostructure devices consisting of alternate InGaAs/InAlAs multilayer stacks (multiquantum wells) have been proposed [21] as potential materials for photoconductive devices and achieve high performance at 1550 nm comparable to LT-GaAs excited at 800 nm. Sartorius
In addition to the GaAs, and InGa(Al)As, many other materials of group III-V such as InAs [23], InSb [23], GaSb [24], GaAsSb [25], and doped InGaAs [26], GaInSb [25] are studied as photoconductive material. Choosing the materials highly depends on the application and operating wavelength. Although LT-GaAs is still the most used material for photoconductive devices and is the most efficient material for 800 nm. However, it exhibits poor absorption at 1.55 μm, where other materials such as InGaAs or InGaAs/InAlAs heterostructure become more attractive. Table 1 summarized some of the photoconductive materials with the advantages, disadvantages, active layer, and the operating wavelength.
Photoconductive material | Advantages | Disadvantages | Active layer | Operating wavelength (nm) |
---|---|---|---|---|
GaAS | The most used materials for THz PCAs and is well studied. It is the most efficient material for 800 nm. | It is not suitable for 1550 nm excitation wavelength. | LT-GaAs | 780 |
LT-GaAs | 770 | |||
LT-GaAs | 776 | |||
LT-GaAs | 800 | |||
SI-GaAs | 800 | |||
GaAs:Er | 1550 | |||
InGaAs | Suitable for 1550 nm excitation wavelength. | Low dark resistivity. | InGaAs | 1550 |
InGaAs | 1550 | |||
Multi-QW | Higher dark resistivity. High performance at 1550 nm comparable to LT-GaAs excited at 800 nm. | More complication. | InGaAs/InAlAs | 1550 |
other materials of group III-V | The ability to engineer the target excitation wavelength. | More complication. It is not well studied. | InAs | 780/ 1550 |
InSb | 780/ 1550 | |||
GaSb | 800 | |||
GaAsSb | 800 (up to 1440) | |||
InGaAs | 800 and 1500 | |||
GaInSb | 800 |
Summary of some photoconductive materials with the advantages, disadvantages, active layer, and the operating wavelength.
The photoconductive devices for THz emission have been developed extensively to fulfill the demand for high-performance THz emitters—and thus be essential for spectroscopic and imaging applications. The development of the emitters’ structure is related to its design and dimensions and how that is attributed to the high performance of the THz emission. The performance of the photoconductive THz emitters is determined in the form of radiated power (or the THz spectral amplitude), SNR, and bandwidth. It is worth noting that the bandwidth here manifests itself as is the maximum frequency in the THz spectral amplitude, as a function of frequency,
In the large-aperture and interdigitated electrodes photoconductive THz emitters, the gap between the two electrodes can be large as 4 mm to 130 μm [11]. Such a gap will allow a high level of optical excitation before reaching the saturation issues. Thus, the importance of such emitters stems from the need to scale up the radiated power, which is influenced by the incident optical power. A molded has been developed by Darrow
In the small-aperture photoconductive THz emitter (dipole antenna), the gap between the two electrodes is smaller than in the large-aperture THz emitters, typically below 200 μm. In this case, it will be more difficult to align the laser spot within the PC gap. Although these emitters experience the saturation issues at lower pump fluence, in comparison with the large-aperture THz emitters, these emitters provide broader bandwidth over the large-aperture THz emitters. Our recent work on the design and structure of photoconductive THz emitters based on SI-GaAs examined the influence of bowtie structure characteristics on the THz spectral amplitude and bandwidth [28]. It is found that the bandwidth can be improved from 3.4 THz to 3.7 THz by changing the design of electrode structure from a sharp bowtie to an asymmetric bowtie structure at the same photoconductive gap. That could be attributed to the smaller capacitance of the sharp bowtie structure over the asymmetric bowtie structure, which results in a shorter resistance-capacitance (RC) time constant. The RC time constant,
Figure 2 illustrates the biased photoconductive gap with its equivalent circuit, here the redistribution of charge on the electrodes, can be seen as incident voltage waveform,
A biased photoconductive gap at bias voltage,
The plasmonic THz emitter is introduced by Berry
A schematic diagram of the photoconductive device shows in (a), the conventional photoconductive THz emitter, and in (b), the plasmonic photoconductive THz emitter. © IOP publishing. Reproduced with permission. All rights reserved [
Overall, the photoconductive structure plays a significant role in the performance of the photoconductive THz emitters. The large-aperture and interdigitated electrodes THz emitters mitigate the influence of saturation for scaling up the THz emission with the optical influence. The small aperture THz emitter (dipole antenna) shows a broader bandwidth, which allows discovering a more comprehensive range of THz frequencies. In addition, the recent studies on plasmonic devices present their significance to the photoconductive THz emitter performance. It also steers the future research and development of high-performance photoconductive devices for spectroscopy, sensing, and imaging applications.
The underlying physics of the THz emission by photoconductive devices is the core of this section, which helps understand these devices’ behavior. The photoconductive THz emission scales linearly with the applied bias field and pump fluence. However, that can be precise only in the ideal case, at low levels of bias field and/or optical excitation. Higher levels of bias field influence the photoconductive THz emitters’ performance. Such influence can be seen as thermal effects, space-charge-limited current effects, etc. In addition, the photoconductive device has a limitation at a higher bias field correlated to the breakdown voltage of the photoconductive material. The pump fluence also has an impact, but that can be observed as the saturation of the THz radiation. The saturation (screening) of the THz radiation is mainly associated with two different mechanisms, being space-charge and near-field screening. This section will explore the limitation of the photoconductive THz emission with insights into the material and structure implications on photoconductive THz emitter’s performance.
The THz radiated power (or the THz field amplitude,
The scaling of THz radiated power as the THz field amplitude,
The pump fluence impacts the radiated THz power in the form of saturation (screening). At a higher level of optical excitation, the radiated THz power will be saturated. This saturation can be classified into two mechanisms, being space-charge and near-field screening. However, each screening status differs based on the photoconductive characteristics (material and structure) and optical characteristics (pump fluence). It is worth noting that transient mobility (mobility as a function of pump fluence) plays an important role in the emitted THz power and thus in the screening of the THz field [30]. The mechanisms of these two screening effects are explained in the next paragraph.
In the space-charge THz screening, the limitation of the photocurrent within the photoconductive gap is due to the high carrier densities within the photoconductive gap, affected by the high pump fluence. The charges drift in the opposite direction. Thus, the bias field screens and ultimately limits the radiated THz field [36]. In the near-field THz screening, the direction of the radiated THz field is in the opposite direction of the bias field, which limits the linear scale of the THz radiated field with the pump fluence, as increasing the pump fluence will raise the carrier densities within the semiconductor [37]. At the same pump fluence, the carrier densities in the emitter with a large photoconductive gap will be smaller than in the emitters with a small photoconductive gap. Thus, a large photoconductive gap emitter leads to scaling up the radiated THz power for higher levels, which increases the total emitter performance, before reaching the screening issues [30].
Overall, the main limitations of the THz emission by photoconductive devices can be related to the applied bias field and the exciting pump fluence. The two limitations are correlated with the photoconductive material and structure characteristics. These two limitations prevent the THz field amplitude from scaling linearly with the bias field and pump fluence. Thus, it is essential to design the photoconductive THz emitter carefully. Furthermore, the photoconductive material must be chosen judiciously to meet the demand of the high-radiated THz field for the aforementioned advanced applications.
A number of the recent advances and research in the field of photoconductive devices are discussed in this section, with insight on the development of the material and structure to enhance the photoconductive THz emission for spectroscopic, sensing, and imaging applications. The section will explore different approaches including:
Quantum dots.
Nanostructured electrodes (non-plasmonic) of the photoconductive device.
Dielectric metasurfaces in photoconductive terahertz devices.
Grating photoconductive devices.
The development of the photoconductive THz emission using such new approaches is notable. The quantum dots are mainly related to photoconductive materials. In contrast, the nanostructured electrodes, dielectric metasurfaces, and Grating photoconductive devices are associated with the photoconductive structure. Here, the main interest is to focus on improving the THz emission using these different approaches and the potential enhancement of these devices.
The quantum dots have been employed to boost the photoconductive THz emitters’ performance. Gorodetsky
Nanostructure electrodes of the photoconductive device show an improvement of the photoconductive THz generation, even without a plasmonic effect. Although the plasmonic photoconductive THz emitter is one of the breakings through in the THz generation and detection field, the nanostructure has its encasement on the performance of such devices [41]. Singh et al. examined an antenna nanostructure fabricated by utilizing an electron-beam lithography system (EBL), having a 5-nm titanium layer and a 25-nm gold layer. Hilbert-fractal design is used with different line widths up to 140 nm. An improvement of the emitted THz power by an approximate factor of two is observed using this nanostructure.
Dielectric metasurfaces in photoconductive terahertz devices can be used as an alternative method to enhance the photoconductive THz emitters’ performance instead of the plasmonic structure [42]. Although the plasmonic structure delivers better THz field improvement over the dielectric structure, the dielectric structure has a substantial characteristic which is the lack of dissipation [43]. In addition, the optical absorption of the incident light (laser) onto the photoconductive device can be improved by reducing the Fresnel losses, which can be done by using thin films of dielectric materials on top of the photoconductive gap. These dielectric materials (thin films) include SiO2, Si3N4, Al2O3, and TiO2 [44, 45]. Figure 5 shows a bowtie antenna having a layer of TiO2 being coated on the photoconductive gap, in (a) the schematic view of the photoconductive THz emitter, (b) the SEM image of the photoconductive THz emitter, and (c) the THz spectral amplitude obtained with using TiO2 layer (red) and without using TiO2 layer (black), “from [45]”.
The bowtie photoconductive antenna with TiO2 layer, coated on the photoconductive gap, in (a) the schematic view of the photoconductive THz emitter, (b) the SEM image of the photoconductive THz emitter, and (c) the THz spectral amplitude obtained with using TiO2 layer (red) and without using TiO2 layer (black). This figure is reprinted from [
The grating structure manifests itself as a periodic array of grooves, lines, slits, etc. The grating structure of the photoconductive devices for THz generation has been studied according to the effective medium approximations (or effective medium theory). The theory can be applied to describe the interaction of light with the grating structure (subwavelength) [46]. Chia et al. have modeled and simulated the influence of grating structure on the THz emission performance by COMSOL Multiphysics software with an insight into the effects of grating geometrical parameters. The author funds an improvement of about 1.63 of the photocurrents obtained by an optimized grating structure of photoconductive THz emitter over the planer emitter structure. This is due to the higher photon absorption, which leads to and leads to more carrier generation within photoconductive material, thus higher photocurrent is observed [46]. Figure 6 shows the simulated grating structure of LT-GaAs and its effects, as in a) the upper diagram shows the surface of planner photoconductive THz emitter, the lower diagram shows grating structure of the photoconductive THz emitter used in the simulation, and b) the normalized electronic concertation obtained by the two different simulated photoconductive THz emitters, “from [46]”.
The simulated grating structure of LT-GaAs, as in (a) the upper diagram shows the surface of planner photoconductive THz emitter, the lower diagram shows grating structure of the photoconductive THz emitter, and (b) the normalized electronic concertation obtained by the two different simulated photoconductive THz emitters. This figure is reprinted from [
Nowadays, the development of photoconductive devices regarding materials and structure is a hot research topic. Several publications have discussed many schemes to achieve higher performance of THz generation by photoconductive devices to facilitate the applications in cutting-edge technologies such as THz spectroscopy, THz sensing, and THz imaging. For photoconductive materials, the research focuses on the quantum dots as well as promotes material properties such as the carrier lifetime and carrier mobility. For the photoconductive structure, the implementation of plasmonic and nanostructures shows its advantage for the aforementioned applications. However, utilizing some novel ideas such as grating structure and a precise selection of the dielectric material is demonstrated to boost the performance of photoconductive devices further.
This chapter presented the photoconductive devices for THz emission. Several materials have been employed as photoconductive materials. However, GaAs is a typical material for these applications, particularly for the sapphire femtosecond pulsed laser sources, which emit at the same range of the bandgap energy of GaAs. Furthermore, several photoconductive structures have been employed. The plasmonic structure shows the highest impact of the photoconductive THz emitters’ performance over the microstructure photoconductive THz emitters. On top of that, the screening effects of the THz field amplitude is an issue limiting the linear scaling of the THz field with the pump fluence. Such limitations can be diminished using a large-aperture photoconductive antenna. At the end of this chapter, the improvement of these devices’ performance has been considered by viewing some recent work in this area. The work has also presented the influence of the quantum dots, the nanostructured electrodes (nonplasmonic) of the photoconductive device, the dielectric materials in photoconductive terahertz devices, and the grating structure on the photoconductive surface. It is hoped that the presented work can lay a role in continuing advancements of photoconductive devices.
The authors declare no conflict of interest.
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Scaffolds",slug:"cell-responses-to-surface-and-architecture-of-tissue-engineering-scaffolds",totalDownloads:10520,totalCrossrefCites:134,totalDimensionsCites:305,abstract:null,book:{id:"314",slug:"regenerative-medicine-and-tissue-engineering-cells-and-biomaterials",title:"Regenerative Medicine and Tissue Engineering",fullTitle:"Regenerative Medicine and Tissue Engineering - Cells and Biomaterials"},signatures:"Hsin-I Chang and Yiwei Wang",authors:[{id:"45747",title:"Dr.",name:"Hsin-I",middleName:null,surname:"Chang",slug:"hsin-i-chang",fullName:"Hsin-I Chang"},{id:"53659",title:"Ms.",name:"Yiwei",middleName:null,surname:"Wang",slug:"yiwei-wang",fullName:"Yiwei Wang"}]},{id:"46479",doi:"10.5772/57353",title:"Floating Drug Delivery Systems for Eradication of Helicobacter pylori in Treatment of Peptic Ulcer Disease",slug:"floating-drug-delivery-systems-for-eradication-of-helicobacter-pylori-in-treatment-of-peptic-ulcer-d",totalDownloads:2864,totalCrossrefCites:139,totalDimensionsCites:302,abstract:null,book:{id:"3839",slug:"trends-in-helicobacter-pylori-infection",title:"Trends in Helicobacter pylori Infection",fullTitle:"Trends in Helicobacter pylori Infection"},signatures:"Yousef Javadzadeh and Sanaz Hamedeyazdan",authors:[{id:"94276",title:"Prof.",name:"Yousef",middleName:null,surname:"Javadzadeh",slug:"yousef-javadzadeh",fullName:"Yousef Javadzadeh"},{id:"98229",title:"Dr.",name:"Sanaz",middleName:null,surname:"Hamedeyazdan",slug:"sanaz-hamedeyazdan",fullName:"Sanaz Hamedeyazdan"}]},{id:"25512",doi:"10.5772/30872",title:"Epidemiology of Psychological Distress",slug:"epidemiology-of-psychological-distress",totalDownloads:8820,totalCrossrefCites:95,totalDimensionsCites:256,abstract:null,book:{id:"727",slug:"mental-illnesses-understanding-prediction-and-control",title:"Mental Illnesses",fullTitle:"Mental Illnesses - Understanding, Prediction and Control"},signatures:"Aline Drapeau, Alain Marchand and Dominic Beaulieu-Prévost",authors:[{id:"84582",title:"Dr.",name:"Aline",middleName:null,surname:"Drapeau",slug:"aline-drapeau",fullName:"Aline Drapeau"},{id:"84605",title:"Dr.",name:"Alain",middleName:null,surname:"Marchand",slug:"alain-marchand",fullName:"Alain Marchand"},{id:"84606",title:"Dr.",name:"Dominic",middleName:null,surname:"Beaulieu-Prévost",slug:"dominic-beaulieu-prevost",fullName:"Dominic Beaulieu-Prévost"}]},{id:"64762",doi:"10.5772/intechopen.82511",title:"Mechanism and Health Effects of Heavy Metal Toxicity in Humans",slug:"mechanism-and-health-effects-of-heavy-metal-toxicity-in-humans",totalDownloads:10461,totalCrossrefCites:107,totalDimensionsCites:248,abstract:"Several heavy metals are found naturally in the earth crust and are exploited for various industrial and economic purposes. Among these heavy metals, a few have direct or indirect impact on the human body. Some of these heavy metals such as copper, cobalt, iron, nickel, magnesium, molybdenum, chromium, selenium, manganese and zinc have functional roles which are essential for various diverse physiological and biochemical activities in the body. However, some of these heavy metals in high doses can be harmful to the body while others such as cadmium, mercury, lead, chromium, silver, and arsenic in minute quantities have delirious effects in the body causing acute and chronic toxicities in humans. The focus of this chapter is to describe the various mechanism of intoxication of some selected heavy metals in humans along with their health effects. Therefore it aims to highlight on biochemical mechanisms of heavy metal intoxication which involves binding to proteins and enzymes, altering their activity and causing damage. More so, the mechanism by which heavy metals cause neurotoxicity, generate free radical which promotes oxidative stress damaging lipids, proteins and DNA molecules and how these free radicals propagate carcinogenesis are discussed. Alongside these mechanisms, the noxious health effects of these heavy metals are discussed.",book:{id:"7111",slug:"poisoning-in-the-modern-world-new-tricks-for-an-old-dog-",title:"Poisoning in the Modern World",fullTitle:"Poisoning in the Modern World - New Tricks for an Old Dog?"},signatures:"Godwill Azeh Engwa, Paschaline Udoka Ferdinand, Friday Nweke Nwalo and Marian N. Unachukwu",authors:[{id:"241837",title:"Mr.",name:"Godwill Azeh",middleName:null,surname:"Engwa",slug:"godwill-azeh-engwa",fullName:"Godwill Azeh Engwa"},{id:"274194",title:"BSc.",name:"Paschaline Ferdinand",middleName:null,surname:"Okeke",slug:"paschaline-ferdinand-okeke",fullName:"Paschaline Ferdinand Okeke"},{id:"286975",title:"Dr.",name:"Friday",middleName:null,surname:"Nweke Nwalo",slug:"friday-nweke-nwalo",fullName:"Friday Nweke Nwalo"},{id:"286976",title:"Dr.",name:"Marian",middleName:null,surname:"Unachukwu",slug:"marian-unachukwu",fullName:"Marian Unachukwu"}]},{id:"27687",doi:"10.5772/29869",title:"Heavy Metals and Human Health",slug:"heavy-metals-and-human-health",totalDownloads:18969,totalCrossrefCites:87,totalDimensionsCites:196,abstract:null,book:{id:"1012",slug:"environmental-health-emerging-issues-and-practice",title:"Environmental Health",fullTitle:"Environmental Health - Emerging Issues and Practice"},signatures:"Simone Morais, Fernando Garcia e Costa and Maria de Lourdes Pereira",authors:[{id:"13875",title:"Prof.",name:"Simone",middleName:null,surname:"Morais",slug:"simone-morais",fullName:"Simone Morais"},{id:"79715",title:"Prof.",name:"Maria De Lourdes",middleName:null,surname:"Pereira",slug:"maria-de-lourdes-pereira",fullName:"Maria De Lourdes Pereira"},{id:"87294",title:"Prof.",name:"Fernando",middleName:null,surname:"Garcia E Costa",slug:"fernando-garcia-e-costa",fullName:"Fernando Garcia E Costa"}]}],mostDownloadedChaptersLast30Days:[{id:"64851",title:"Herbal Medicines in African Traditional Medicine",slug:"herbal-medicines-in-african-traditional-medicine",totalDownloads:14512,totalCrossrefCites:33,totalDimensionsCites:56,abstract:"African traditional medicine is a form of holistic health care system organized into three levels of specialty, namely divination, spiritualism, and herbalism. The traditional healer provides health care services based on culture, religious background, knowledge, attitudes, and beliefs that are prevalent in his community. Illness is regarded as having both natural and supernatural causes and thus must be treated by both physical and spiritual means, using divination, incantations, animal sacrifice, exorcism, and herbs. Herbal medicine is the cornerstone of traditional medicine but may include minerals and animal parts. The adjustment is ok, but may be replaced with –‘ Herbal medicine was once termed primitive by western medicine but through scientific investigations there is a better understanding of its therapeutic activities such that many pharmaceuticals have been modeled on phytochemicals derived from it. Major obstacles to the use of African medicinal plants are their poor quality control and safety. Traditional medical practices are still shrouded with much secrecy, with few reports or documentations of adverse reactions. However, the future of African traditional medicine is bright if viewed in the context of service provision, increase of health care coverage, economic potential, and poverty reduction. Formal recognition and integration of traditional medicine into conventional medicine will hold much promise for the future.",book:{id:"6302",slug:"herbal-medicine",title:"Herbal Medicine",fullTitle:"Herbal Medicine"},signatures:"Ezekwesili-Ofili Josephine Ozioma and Okaka Antoinette Nwamaka\nChinwe",authors:[{id:"191264",title:"Prof.",name:"Josephine",middleName:"Ozioma",surname:"Ozioma Ezekwesili-Ofili",slug:"josephine-ozioma-ezekwesili-ofili",fullName:"Josephine Ozioma Ezekwesili-Ofili"},{id:"211585",title:"Prof.",name:"Antoinette",middleName:null,surname:"Okaka",slug:"antoinette-okaka",fullName:"Antoinette Okaka"}]},{id:"76640",title:"Control of Clinical Laboratory Errors by FMEA Model",slug:"control-of-clinical-laboratory-errors-by-fmea-model",totalDownloads:1208,totalCrossrefCites:0,totalDimensionsCites:0,abstract:"Patient safety is an aim for clinical applications and is a fundamental principle of healthcare and quality management. The main global health organizations have incorporated patient safety in their review of work practices. The data provided by the medical laboratories have a direct impact on patient safety and a fault in any of processes such as strategic, operational and support, could affect it. To provide appreciate and reliable data to the physicians, it is important to emphasize the need to design risk management plan in the laboratory. Failure Mode and Effect Analysis (FMEA) is an efficient technique for error detection and reduction. Technical Committee of the International Organization for Standardization (ISO) licensed a technical specification for medical laboratories suggesting FMEA as a method for prospective risk analysis of high-risk processes. FMEA model helps to identify quality failures, their effects and risks with their reduction/elimination, which depends on severity, probability and detection. Applying FMEA in clinical approaches can lead to a significant reduction of the risk priority number (RPN).",book:{id:"9808",slug:"contemporary-topics-in-patient-safety-volume-1",title:"Contemporary Topics in Patient Safety",fullTitle:"Contemporary Topics in Patient Safety - Volume 1"},signatures:"Hoda Sabati, Amin Mohsenzadeh and Nooshin Khelghati",authors:[{id:"340486",title:"M.Sc.",name:"Hoda",middleName:null,surname:"Sabati",slug:"hoda-sabati",fullName:"Hoda Sabati"},{id:"348872",title:"M.Sc.",name:"Amin",middleName:null,surname:"Mohsenzadeh",slug:"amin-mohsenzadeh",fullName:"Amin Mohsenzadeh"},{id:"348874",title:"MSc.",name:"Nooshin",middleName:null,surname:"Khelghati",slug:"nooshin-khelghati",fullName:"Nooshin Khelghati"}]},{id:"64762",title:"Mechanism and Health Effects of Heavy Metal Toxicity in Humans",slug:"mechanism-and-health-effects-of-heavy-metal-toxicity-in-humans",totalDownloads:10456,totalCrossrefCites:107,totalDimensionsCites:242,abstract:"Several heavy metals are found naturally in the earth crust and are exploited for various industrial and economic purposes. Among these heavy metals, a few have direct or indirect impact on the human body. Some of these heavy metals such as copper, cobalt, iron, nickel, magnesium, molybdenum, chromium, selenium, manganese and zinc have functional roles which are essential for various diverse physiological and biochemical activities in the body. However, some of these heavy metals in high doses can be harmful to the body while others such as cadmium, mercury, lead, chromium, silver, and arsenic in minute quantities have delirious effects in the body causing acute and chronic toxicities in humans. The focus of this chapter is to describe the various mechanism of intoxication of some selected heavy metals in humans along with their health effects. Therefore it aims to highlight on biochemical mechanisms of heavy metal intoxication which involves binding to proteins and enzymes, altering their activity and causing damage. More so, the mechanism by which heavy metals cause neurotoxicity, generate free radical which promotes oxidative stress damaging lipids, proteins and DNA molecules and how these free radicals propagate carcinogenesis are discussed. Alongside these mechanisms, the noxious health effects of these heavy metals are discussed.",book:{id:"7111",slug:"poisoning-in-the-modern-world-new-tricks-for-an-old-dog-",title:"Poisoning in the Modern World",fullTitle:"Poisoning in the Modern World - New Tricks for an Old Dog?"},signatures:"Godwill Azeh Engwa, Paschaline Udoka Ferdinand, Friday Nweke Nwalo and Marian N. Unachukwu",authors:[{id:"241837",title:"Mr.",name:"Godwill Azeh",middleName:null,surname:"Engwa",slug:"godwill-azeh-engwa",fullName:"Godwill Azeh Engwa"},{id:"274194",title:"BSc.",name:"Paschaline Ferdinand",middleName:null,surname:"Okeke",slug:"paschaline-ferdinand-okeke",fullName:"Paschaline Ferdinand Okeke"},{id:"286975",title:"Dr.",name:"Friday",middleName:null,surname:"Nweke Nwalo",slug:"friday-nweke-nwalo",fullName:"Friday Nweke Nwalo"},{id:"286976",title:"Dr.",name:"Marian",middleName:null,surname:"Unachukwu",slug:"marian-unachukwu",fullName:"Marian Unachukwu"}]},{id:"65467",title:"Anesthesia Management for Large-Volume Liposuction",slug:"anesthesia-management-for-large-volume-liposuction",totalDownloads:6203,totalCrossrefCites:1,totalDimensionsCites:2,abstract:"The apparent easiness with which liposuction is performed favors that patients, young surgeons, and anesthesiologists without experience in this field ignore the many events that occur during this procedure. Liposuction is a procedure to improve the body contour and not a surgery to reduce weight, although recently people who have failed in their plans to lose weight look at liposuction as a means to contour their body figure. Tumescent liposuction of large volumes requires a meticulous selection of each patient; their preoperative evaluation and perioperative management are essential to obtain the expected results. The various techniques of general anesthesia are the most recommended and should be monitored in the usual way, as well as monitoring the total doses of infiltrated local anesthetics to avoid systemic toxicity. The management of intravenous fluids is controversial, but the current trend is the restricted use of hydrosaline solutions. The most feared complications are deep vein thrombosis, pulmonary thromboembolism, fat embolism, lung edema, hypothermia, infections and even death. The adherence to the management guidelines and prophylaxis of venous thrombosis/thromboembolism is mandatory.",book:{id:"6221",slug:"anesthesia-topics-for-plastic-and-reconstructive-surgery",title:"Anesthesia Topics for Plastic and Reconstructive Surgery",fullTitle:"Anesthesia Topics for Plastic and Reconstructive Surgery"},signatures:"Sergio Granados-Tinajero, Carlos Buenrostro-Vásquez, Cecilia\nCárdenas-Maytorena and Marcela Contreras-López",authors:[{id:"273532",title:"Dr.",name:"Sergio Octavio",middleName:null,surname:"Granados Tinajero",slug:"sergio-octavio-granados-tinajero",fullName:"Sergio Octavio Granados Tinajero"}]},{id:"30178",title:"Chest Mobilization Techniques for Improving Ventilation and Gas Exchange in Chronic Lung Disease",slug:"chest-mobilization-techniques-for-improving-ventilation-and-gas-exchange-in-chronic-lung-disease",totalDownloads:31227,totalCrossrefCites:0,totalDimensionsCites:5,abstract:null,book:{id:"648",slug:"chronic-obstructive-pulmonary-disease-current-concepts-and-practice",title:"Chronic Obstructive Pulmonary Disease",fullTitle:"Chronic Obstructive Pulmonary Disease - Current Concepts and Practice"},signatures:"Donrawee Leelarungrayub",authors:[{id:"73709",title:"Associate Prof.",name:"Jirakrit",middleName:null,surname:"Leelarungrayub",slug:"jirakrit-leelarungrayub",fullName:"Jirakrit Leelarungrayub"}]}],onlineFirstChaptersFilter:{topicId:"3",limit:6,offset:0},onlineFirstChaptersCollection:[{id:"83000",title:"Purine and Pyrimidine Pathways as Antimalarial Targets",slug:"purine-and-pyrimidine-pathways-as-antimalarial-targets",totalDownloads:1,totalDimensionsCites:null,doi:"10.5772/intechopen.106468",abstract:"Malaria continues to plague the endemic regions of sub-Saharan Africa and Southeast Asia. With the current development of artemisinin resistance and a risk of failure of the current first line therapies, there is a growing need for novel antimalarials. Purine and pyrimidine metabolism in Plasmodium is distinctly different from the human host, making these pathways valid targets for the development of novel antimalarials. Targeting key enzymes in these pathways with transition state analogs has provided high affinity inhibitors. Transition state mimicry can also provide selectivity for the parasite enzymes over the homologous enzymes of the human host. Resistance of Plasmodium parasites to current antimalarials will be compared to resistance development induced by transition state analogs inhibitors, a feature that may contribute to decreased resistance development. Tight binding and specificity of transition state analog inhibitors provide important features for novel antimalaria therapy with low toxicity and prevention of antibiotic resistance.",book:{id:"11576",title:"Malaria - Recent Advances, and New Perspectives",coverURL:"https://cdn.intechopen.com/books/images_new/11576.jpg"},signatures:"Yacoba V.T. Minnow and Vern L. Schramm"},{id:"82264",title:"Understand Sphingolipids Metabolism in Colorectal Cancer",slug:"understand-sphingolipids-metabolism-in-colorectal-cancer",totalDownloads:1,totalDimensionsCites:null,doi:"10.5772/intechopen.105465",abstract:"Colorectal cancer is the fourth most frequently diagnosed cancer and one of the leading causes of cancer death around the world. Patients with locally advanced rectal cancer are treated with a combination of radiotherapy, chemotherapy, and surgery. Treatment response can be quite variable—some with complete response, while others show little or no response—and pathologic response has become a significant predictor of good oncologic outcome. The knowledge of the molecular pathways in colorectal cancer is increasing. However, unfortunately, it still fails to find some more precise method to select and tailor patients to different treatment approaches and overcome treatment resistance. Recent investigations showed that sphingolipids play an essential role in cancer biology and can influence treatment response and aggressiveness. It is of utmost importance to understand sphingolipids’ metabolism in colorectal cancer and how it affects tumor biology and response to treatment.",book:{id:"11595",title:"Recent Understanding of Colorectal Cancer Treatment",coverURL:"https://cdn.intechopen.com/books/images_new/11595.jpg"},signatures:"Pedro Nuno Brandão, Lúcia Lacerda and Marisa D. Santos"},{id:"82077",title:"Cultivation Practice of Chinese Medicinal Herbs",slug:"cultivation-practice-of-chinese-medicinal-herbs",totalDownloads:1,totalDimensionsCites:0,doi:"10.5772/intechopen.104859",abstract:"An innovative cultivation technique for Chinese medicinal herbs had been practiced in China, which led a new road for medicinal herbs production without input of chemical fertilizer and chemical pesticides. The organic practice was based on the principle of biodiversity for pest control. An example of Panax notoginseng (Burk.) F. H. Chen was chosen for explaining cultivation technology under forest. The key technologies for P. notoginseng cultivation under forest include forest land selection, land tillage, seedling breeding and transplanting, and on-farm organic management. These technologies can standardize herbs production in large-scale under forest, and the quality and safety of P. notoginseng can be effectively improved without applying chemical pesticides and chemical fertilizer in the production process.",book:{id:"11299",title:"Medicinal Plants",coverURL:"https://cdn.intechopen.com/books/images_new/11299.jpg"},signatures:"Xiahong He, Kuan Yang, Shusheng Zhu, Liwei Guo and Chen Ye"},{id:"82615",title:"Intracorporeal Urinary Diversion of Robot-Assisted Radical Cystectomy",slug:"intracorporeal-urinary-diversion-of-robot-assisted-radical-cystectomy",totalDownloads:0,totalDimensionsCites:0,doi:"10.5772/intechopen.105980",abstract:"With the widespread utilization of robot-assisted radical cystectomy (RARC) that demonstrated non-inferiority compared to open radical cystectomy in terms of several outcomes, urinary diversions are now performed for both extracorporeal and intracorporeal procedures. The potential benefits of intracorporeal urinary diversion (ICUD) include smaller incisions, reduced pain, reduced intraoperative blood loss, reduced bowel handling and exposure, and third space loss. ICUD following radical cystectomy requires many steps and a careful stepwise progression. Surgical volumes (RARCs per year) per center and per surgeon appear to be correlated with a reduction in complications. The European Association of Urology guidelines recommend that hospitals should perform at least 10, and preferably more than 20 operations annually. With the aim of generalizing ICUD, this chapter will discuss the following items: (1) Technique of intracorporeal ileal conduit; (2) Perioperative comparison of intracorporeal and extracorporeal urinary diversion in RARC; (3) Hybrid technique in robot-assisted intracorporeal ileal conduit; and (4) Intracorporeal ileal neobladder.",book:{id:"11886",title:"Bladder Cancer",coverURL:"https://cdn.intechopen.com/books/images_new/11886.jpg"},signatures:"Yasukazu Nakanishi, Shugo Yajima and Hitoshi Masuda"},{id:"83087",title:"Role of Cellular Responses in Periodontal Tissue Destruction",slug:"role-of-cellular-responses-in-periodontal-tissue-destruction",totalDownloads:4,totalDimensionsCites:0,doi:"10.5772/intechopen.106645",abstract:"Periodontal tissue destruction is the deterioration of tooth-supporting components, particularly the periodontal ligament (PDL) and alveolar bone, resulting in gingival recession, root exposure, tooth mobility and drifting, and, finally, tooth loss. The breakdown of the epithelial barriers by infection or mechanical damage allows bacteria and their toxins to enter and stimulates the immune response. The bacteria cause periodontal damage via the cascade of the host reaction which is crucial in the destruction of the connective tissue around the tooth. The OPG/RANKL/RANK system is the key player in bone regulation of periodontal tissue and was controlled by both immune and non-immune cells. This knowledge has predicated the successfulness of implant and orthodontics treatments with the predictable healing and regeneration of the bone and supporting tissues surrounding the teeth.",book:{id:"11566",title:"Periodontology - New Insights",coverURL:"https://cdn.intechopen.com/books/images_new/11566.jpg"},signatures:"Nam Cong-Nhat Huynh"},{id:"83086",title:"Therapeutic Options in Graves’ Hyperthyroidism",slug:"therapeutic-options-in-graves-hyperthyroidism",totalDownloads:7,totalDimensionsCites:0,doi:"10.5772/intechopen.106562",abstract:"The classical approach to treating Graves’ hyperthyroidism involves rapid control of the symptoms, generally with a beta adrenergic blocker, and reduction of thyroid hormone secretion by antithyroid drugs (ATDs) and/or using one of the several modalities available, including radioactive iodine therapy (RAI), and surgery; the selection of the treatment modalities often varies according to different guidelines, patient preferences and local traditions. Thionamides are invariably used as first-line medication to control hyperthyroidism and induce remission of the disease, thereby relieving the symptoms. In case of failure of the medical therapy, which is not uncommon, definitive treatment with surgery or RAI is the standard modality of management after due consideration and discussion with the patients. However, the therapeutic options available for patients with Graves’ hyperthyroidism have remained largely unchanged for the past several decades despite the current treatments having either limited efficacy or significant adverse effects. The clinical demand for new therapeutic regimens of Graves’ disease has led to the emergence of several new therapeutic ideas/options like biologic, peptide immunomodulation and small molecules, currently under investigations which may lead to the restoration of a euthyroid state without the requirement for ongoing therapy, but the potential risk of immunocompromise and cost implications needs careful consideration.",book:{id:"11712",title:"Hyperthyroidism - Recent Updates",coverURL:"https://cdn.intechopen.com/books/images_new/11712.jpg"},signatures:"Javaid Ahmad Bhat, Shoiab Mohd Patto, Pooran Sharma, Mohammad Hayat Bhat and Shahnaz Ahmad Mir"}],onlineFirstChaptersTotal:834},preDownload:{success:null,errors:{}},subscriptionForm:{success:null,errors:{}},aboutIntechopen:{},privacyPolicy:{},peerReviewing:{},howOpenAccessPublishingWithIntechopenWorks:{},sponsorshipBooks:{sponsorshipBooks:[],offset:0,limit:8,total:null},allSeries:{pteSeriesList:[{id:"14",title:"Artificial Intelligence",numberOfPublishedBooks:9,numberOfPublishedChapters:90,numberOfOpenTopics:6,numberOfUpcomingTopics:0,issn:"2633-1403",doi:"10.5772/intechopen.79920",isOpenForSubmission:!0},{id:"7",title:"Biomedical Engineering",numberOfPublishedBooks:12,numberOfPublishedChapters:108,numberOfOpenTopics:3,numberOfUpcomingTopics:0,issn:"2631-5343",doi:"10.5772/intechopen.71985",isOpenForSubmission:!0}],lsSeriesList:[{id:"11",title:"Biochemistry",numberOfPublishedBooks:33,numberOfPublishedChapters:330,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2632-0983",doi:"10.5772/intechopen.72877",isOpenForSubmission:!0},{id:"25",title:"Environmental Sciences",numberOfPublishedBooks:1,numberOfPublishedChapters:19,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2754-6713",doi:"10.5772/intechopen.100362",isOpenForSubmission:!0},{id:"10",title:"Physiology",numberOfPublishedBooks:14,numberOfPublishedChapters:145,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2631-8261",doi:"10.5772/intechopen.72796",isOpenForSubmission:!0}],hsSeriesList:[{id:"3",title:"Dentistry",numberOfPublishedBooks:9,numberOfPublishedChapters:141,numberOfOpenTopics:2,numberOfUpcomingTopics:0,issn:"2631-6218",doi:"10.5772/intechopen.71199",isOpenForSubmission:!0},{id:"6",title:"Infectious Diseases",numberOfPublishedBooks:13,numberOfPublishedChapters:124,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2631-6188",doi:"10.5772/intechopen.71852",isOpenForSubmission:!0},{id:"13",title:"Veterinary Medicine and Science",numberOfPublishedBooks:11,numberOfPublishedChapters:112,numberOfOpenTopics:3,numberOfUpcomingTopics:0,issn:"2632-0517",doi:"10.5772/intechopen.73681",isOpenForSubmission:!0}],sshSeriesList:[{id:"22",title:"Business, Management and Economics",numberOfPublishedBooks:1,numberOfPublishedChapters:22,numberOfOpenTopics:3,numberOfUpcomingTopics:0,issn:"2753-894X",doi:"10.5772/intechopen.100359",isOpenForSubmission:!0},{id:"23",title:"Education and Human Development",numberOfPublishedBooks:0,numberOfPublishedChapters:11,numberOfOpenTopics:1,numberOfUpcomingTopics:1,issn:null,doi:"10.5772/intechopen.100360",isOpenForSubmission:!0},{id:"24",title:"Sustainable Development",numberOfPublishedBooks:1,numberOfPublishedChapters:19,numberOfOpenTopics:5,numberOfUpcomingTopics:0,issn:"2753-6580",doi:"10.5772/intechopen.100361",isOpenForSubmission:!0}],testimonialsList:[{id:"13",text:"The collaboration with and support of the technical staff of IntechOpen is fantastic. 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Biochemistry examines macromolecules - proteins, nucleic acids, carbohydrates, and lipids – and their building blocks, structures, functions, and interactions. Much of biochemistry is devoted to enzymes, proteins that catalyze chemical reactions, enzyme structures, mechanisms of action and their roles within cells. Biochemistry also studies small signaling molecules, coenzymes, inhibitors, vitamins, and hormones, which play roles in life processes. Biochemical experimentation, besides coopting classical chemistry methods, e.g., chromatography, adopted new techniques, e.g., X-ray diffraction, electron microscopy, NMR, radioisotopes, and developed sophisticated microbial genetic tools, e.g., auxotroph mutants and their revertants, fermentation, etc. More recently, biochemistry embraced the ‘big data’ omics systems. Initial biochemical studies have been exclusively analytic: dissecting, purifying, and examining individual components of a biological system; in the apt words of Efraim Racker (1913 –1991), “Don’t waste clean thinking on dirty enzymes.” Today, however, biochemistry is becoming more agglomerative and comprehensive, setting out to integrate and describe entirely particular biological systems. The ‘big data’ metabolomics can define the complement of small molecules, e.g., in a soil or biofilm sample; proteomics can distinguish all the comprising proteins, e.g., serum; metagenomics can identify all the genes in a complex environment, e.g., the bovine rumen. 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Her research interests include archaea metabolism, enzymes purification and characterization, gene regulation, carotenoids and bioplastics production, antioxidant\ncompounds, waste water treatments, and brines bioremediation.\nRosa María’s other roles include editorial board member for several journals related\nto biochemistry, reviewer for more than 60 journals (biochemistry, molecular biology, biotechnology, chemistry and microbiology) and president of several organizing committees in international meetings related to the N-cycle or respiratory processes.",institutionString:null,institution:{name:"University of Alicante",institutionURL:null,country:{name:"Spain"}}},editorTwo:null,editorThree:null},{id:"15",title:"Chemical Biology",coverUrl:"https://cdn.intechopen.com/series_topics/covers/15.jpg",isOpenForSubmission:!0,editor:{id:"441442",title:"Dr.",name:"Şükrü",middleName:null,surname:"Beydemir",slug:"sukru-beydemir",fullName:"Şükrü Beydemir",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0033Y00003GsUoIQAV/Profile_Picture_1634557147521",biography:"Dr. Şükrü Beydemir obtained a BSc in Chemistry in 1995 from Yüzüncü Yıl University, MSc in Biochemistry in 1998, and PhD in Biochemistry in 2002 from Atatürk University, Turkey. 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He is especially interested in the genetic differentiation pattern and speciation process that correlate to the flashing pattern and mating behavior of some fireflies in Japan. He then worked for Olympus Corporation, a Japanese manufacturer of optics and imaging products, where he was involved in the development of luminescence technology and produced a bioluminescence microscope that is currently being used for gene expression analysis in chronobiology, neurobiology, and developmental biology. 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