Summary of some photoconductive materials with the advantages, disadvantages, active layer, and the operating wavelength.
\\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:"175",leadTitle:null,fullTitle:"Nanocrystal",title:"Nanocrystal",subtitle:null,reviewType:"peer-reviewed",abstract:'We focused on cutting-edge science and technology of Nanocrystals in this book. "Nanocrystal" is expected to lead to the creation of new materials with revolutionary properties and functions. It will open up fresh possibilities for the solution to the environmental problems and energy problems. We wish that this book contributes to bequeath a beautiful environment and valuable resources to subsequent generations.',isbn:null,printIsbn:"978-953-307-199-2",pdfIsbn:"978-953-51-5538-6",doi:"10.5772/703",price:159,priceEur:175,priceUsd:205,slug:"nanocrystal",numberOfPages:506,isOpenForSubmission:!1,isInWos:null,isInBkci:!1,hash:"be72531b15b9a96a9eebf85b56a9e0d4",bookSignature:"Yoshitake Masuda",publishedDate:"June 28th 2011",coverURL:"https://cdn.intechopen.com/books/images_new/175.jpg",numberOfDownloads:74023,numberOfWosCitations:65,numberOfCrossrefCitations:22,numberOfCrossrefCitationsByBook:3,numberOfDimensionsCitations:71,numberOfDimensionsCitationsByBook:5,hasAltmetrics:1,numberOfTotalCitations:158,isAvailableForWebshopOrdering:!0,dateEndFirstStepPublish:"October 11th 2010",dateEndSecondStepPublish:"November 8th 2010",dateEndThirdStepPublish:"February 13th 2011",dateEndFourthStepPublish:"April 14th 2011",dateEndFifthStepPublish:"June 28th 2011",currentStepOfPublishingProcess:5,indexedIn:"1,2,3,4,5,6,7",editedByType:"Edited by",kuFlag:!1,featuredMarkup:null,editors:[{id:"12385",title:"Dr.",name:"Yoshitake",middleName:null,surname:"Masuda",slug:"yoshitake-masuda",fullName:"Yoshitake Masuda",profilePictureURL:"https://mts.intechopen.com/storage/users/12385/images/1862_n.jpg",biography:"Dr. Yoshitake Masuda is a senior research scientist at the National Institute of Advanced Industrial Science and Technology (AIST), Japan. He graduated from Tsukuba University in 1994, and received his Master of Engineering degree from Tsukuba University in 1996. He was an engineer at NGK Spark Plug Co. Ltd., from 1996 to 1998, and an assistant professor at Nagoya University from 2000 to 2006. Dr. Masuda received his Doctor of Engineering degree from Nagoya University in 2004, and his PhD thesis was on the Patterning of TiO2 Thin Films and Particles using Self-assembled Monolayers.",institutionString:null,position:null,outsideEditionCount:0,totalCites:0,totalAuthoredChapters:"6",totalChapterViews:"0",totalEditedBooks:"3",institution:{name:"Nagoya University",institutionURL:null,country:{name:"Japan"}}}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,coeditorOne:null,coeditorTwo:null,coeditorThree:null,coeditorFour:null,coeditorFive:null,topics:[{id:"1169",title:"Condensed Matter Physics",slug:"nanotechnology-and-nanomaterials-material-science-condensed-matter-physics"}],chapters:[{id:"15874",title:"Morphology Control of Metal Oxide Nanocrystals",doi:"10.5772/23352",slug:"morphology-control-of-metal-oxide-nanocrystals",totalDownloads:4570,totalCrossrefCites:0,totalDimensionsCites:2,hasAltmetrics:0,abstract:null,signatures:"Yoshitake Masuda",downloadPdfUrl:"/chapter/pdf-download/15874",previewPdfUrl:"/chapter/pdf-preview/15874",authors:[{id:"12385",title:"Dr.",name:"Yoshitake",surname:"Masuda",slug:"yoshitake-masuda",fullName:"Yoshitake Masuda"}],corrections:null},{id:"15875",title:"Size- and Shape-Controlled Synthesis of Monodisperse Metal Oxide and Mixed Oxide Nanocrystals",doi:"10.5772/17054",slug:"size-and-shape-controlled-synthesis-of-monodisperse-metal-oxide-and-mixed-oxide-nanocrystals",totalDownloads:13932,totalCrossrefCites:6,totalDimensionsCites:18,hasAltmetrics:0,abstract:null,signatures:"Thanh-Dinh Nguyen and Trong-On Do",downloadPdfUrl:"/chapter/pdf-download/15875",previewPdfUrl:"/chapter/pdf-preview/15875",authors:[{id:"27116",title:"Prof.",name:"Trong-On",surname:"Do",slug:"trong-on-do",fullName:"Trong-On Do"},{id:"44088",title:"Dr.",name:"Thanh-Dinh",surname:"Nguyen",slug:"thanh-dinh-nguyen",fullName:"Thanh-Dinh Nguyen"}],corrections:null},{id:"15876",title:"Colloidal Hybrid Nanocrystals: Synthesis, Properties, and Perspectives",doi:"10.5772/16418",slug:"colloidal-hybrid-nanocrystals-synthesis-properties-and-perspectives",totalDownloads:5117,totalCrossrefCites:0,totalDimensionsCites:4,hasAltmetrics:0,abstract:null,signatures:"Jie Zeng, Xiaoping Wang and J. 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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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