Salinity tolerant cultivars of Brassica species developed through conventional breeding.
\r\n\tUnstoppable progress in the technologies of synthesis of diamond, graphene, and its compounds with stable parameters will provide materials for the industry of devices for integrated, radio, Opto- and quantum electronics and photonics.
\r\n\tIn most electronic and optical properties, diamond and graphene are superior to traditional and perspective semiconductors. It is safe to say that silicon and gallium arsenide are materials for electronics and optoelectronics of the past, gallium nitride and silicon carbide are high-tech today, and diamond and graphene are the future of electronics and photonics.
Globally the total area of saline soil is 397 million ha and 434 million ha of sodic soil. Of the 230 million irrigated fields, 45 million ha (19.5%) are salt-affected and almost 1500 million ha of arable agriculture, 32 million (2.1%) salt-affected [1]. Of the world’s salt-affected land, an estimated 6.73 million ha are in India. In addition, arid and semi-arid areas are associated with salty groundwater, which must be used for irrigation, due to the unavailability or diversion of quality water outside for agricultural purposes. The use of this salty groundwater makes the soil unsuitable for growing crops. Salt stress is currently one of the most critical factors, reducing agricultural production (Figure 1).
View of natural salt affected soil.
Reclamation of these salt affected areas is of paramount importance to bring more and more areas under cultivation. This is necessary to enhance the food availability for feeding the burgeoning population in the country. Generally, there are three approaches being followed for the reclamation of these salt affected soils. Of these, the engineering solution is beyond the reach of resource poor farmers due to its prohibitive cost and community based application. The chemical amendment approach is generally followed by the farmers, even for which the subsidies are required to be provided by the Governmental agencies. Further, the smaller land holdings with the resource poor farmers also act as a deterrent in the adoption of these technologies. Thirdly, the biological reclamation approach, by developing salinity and alkalinity tolerant crops, is cost effective and is also economically feasible.
Vast literature is available on the effects of salinity on crop plants. Higher amount of salt reduces the productivity of many agricultural crops [2]; salt stress has three way effects that reduce water potential and cause ion toxicity and imbalances [3]. Salt stress affects other major processes such as germination, germination speed, root/shoot dry weight and the Na+/K+ in the root and shoot [4]. Hence, salt tolerance is important during the life cycle of any plants. Excessive salinity reduces the productivity of many agricultural crops [2], Salt stress has three fold effects which reduces water potential and causes ion imbalance and toxicity [3]. These studies have revealed the complex and polygenic nature of plant salt tolerance. Potential of genetic approach towards solving the problems of soil salinity and alkalinity is now widely recognized and this approach may more relevant to areas that often facing hard constraints of availability of resources. The existence of sufficient heritable variability may help for Genetic adaptation of crops to salinity which permits the identification and selection of salt tolerant strains and traits confer salt tolerance. Modern varieties have a relatively narrow genetic base and are poorly adapted to adverse environments such as salinity. However, endemic genotypes from problem environments may provide the basic germplasm for breeding salt tolerant varieties with acceptable yield potentials. Notwithstanding, the, genetic variations for salt tolerance among agricultural crops are very less, because most of the cultivated genotypes have been selected from normal environment where salt tolerant traits must have been gradually discarded, however variability for salt tolerance are similar in many wild progenitors due to where natural selection in response to salty habitats.
Large amount of variability is present amongst different crops with respect to their behavior under salt stress and this has also been documented. Further, variability is also available within a particular crop for their performance under varying rootzone salinity. The availability of such kind of variability in a crop is an essential requirement for the improvement in its salt tolerance character besides retaining or incorporating the other desirable beneficial characters. Further, the pool of variability in any crop can also be enhanced by subjecting them to mutagenic agents, which can further be screened for the desired characters. Screening whole plants and the large amount of germplasm available for a particular crop for salinity tolerance in the field situations is really time consuming, labour intensive and herculean task. Keeping these factors in view, rapid screening methodologies have also been developed for screening large number of germplasm for salinity tolerance under solution culture in laboratory conditions. When plant breeders are faced with a task of breeding crop varieties which are to be used under specific problem conditions, the criteria of selection is essential to any advancement which may be possible. In case of salt resistance, it would seem that it is essential to work hand to hand with the plant physiologists and soil scientists, in conditions which would make reliable selection possible and to determine if parameters can be developed which can make selection possible and effective. Further, without a concerted and concentrated research effort, problem such as breeding for salt tolerance cannot be effectively pursued.
Brassicas are an important group of edible oil and vegetable plants of the Brassicaceae family. The group has six cultivated species, namely,
The Triangle of U diagram shows the genetic relationship between the six species of the genus Brassica. Three of the Brassica species were derived from three ancestral genomes, denoted by the letters AA (
Brassicas is the third most important edible oil source in the world, after soybean and palm, grown in more than 50 countries around the world. China, Canada, India, Germany, France, UK, Australia, Poland and the USA are the major producers of various varieties of Brassica. Globally, India accounts for 21.7% and production area 10.7% [1]. In India, oil-seed Brassicas are cultivated at about 2.3 million ha salt affected fields out of 6.9 million total cultivated area, which fall under the arid region, affected by varying levels of saline soils [5].
In addition, unhealthy nutritional imbalances due to stress-induced nutrient uptake; depletion in the germination, chlorophyll and mineral ions slow down seed growth and early crop maturity under high salt intake can be attributed to reduced oil content [8, 9]. Further the salinity also significantly reduced net photosynthesis, stomatal conductance, water use efficiency and transpiration under during the formation of siliqua results in the greater yield loss [10].
Higher salt (EC > 12 dS/m); decreased the oil, protein and crude fiber content by 5–7%, 15–20% and 29–34% respectively, while the content of erucic acid increased by 12–17% [5]. However, its growth and productivity are greatly reduced by salt. This situation can be mitigated in a way that includes water conservation and irrigation, crop management and crop production. There is a great deal of interest in the breeding stress-tolerant species, because significant genetic variations for salt tolerance exist between and within Brassica, which requires being exploited by selection and breeding. However, programs to develop salt tolerance species are hampered by traits complexity, inadequate genetic and physiological knowledge of tolerance-related factors, and a lack of an effective selection background. Improved mustard varieties with high salt tolerance and consumer accepted oil quality are required to achieve high yields and to increase the cultivated area under this stressful environment.
Salt tolerance is a complex characteristics that you can learn for the following reasons: (a) salt tolerance can only be tested under stressful conditions, which can affect many plant responses; (b) salt tolerance is a quantitative factor that requires effective and efficient methods of quantifying tolerance levels; (c) “salt” in “salt stress” is often misunderstood as it may contain different mineral salts, such as NaCl, MgCl2, and CaCl2; without excessive use of NaCl in salt, we cannot ignore the damage due to other ions; and (d) other abiotic stresses like drought, excess acidity and alkalinity, are often associated with salt exposed plants, making this difficult to study. Therefore, effective and efficient methods should be used, including plant culture under salt conditions, characterization and quantification of a salt tolerance level, in the first phase of the study.
Plants that grow under certain controlled conditions (e.g. hydroponics) are often used for salt tolerance studies because there is very little natural saline soil that can provide a representative and stable environment [11]. Large pots under the controlled conditions (Microplots/hydroponics) required for growth of Brassica plants and seedlings, while very less experiments for yield evaluation have been conducted in salt affected land. It is noteworthy that the salt tolerance of the Brassicas may be determined by a variety of genes, expressed by salt tolerance responses at various stages of development [12, 13, 14, 15].
Diversification of locations, maximization of replications and monitoring of the environmental conditions during crop growth often provide a good control over the factors responsible for performance of a genotype or a set of genotypes. At ICAR-Central Soil Salinity Research Institute (ICAR-CSSRI), for large scale screening of varieties at germination and seedling stage, shallow-depth germination trays provided with a polythene sheet lining on the inner face are being used. They allow a simulation of germination response of the field nature, giving not only a quantitative indication of relative germination and survival rates but also the relative delays in germination, which is a characteristic of the different genotypes under salinity as well as sodicity stress. Apart from this, microplots of various sizes were constructed at the Institute filled with artificially prepared saline soil or original salty soil brought from salt affected fields, so that soil is uniform all through the profile. This way desired level of sodicity and salinity in these microplots can be maintained uniformly. Data obtained from microplots containing desired levels of saline or alkali soils, have been found to be well correlated with those collected from satisfactorily conducted field experiments. The field gradient of soil salinity is determined by soil tests at small intervals of space and a long strip running full length across the salinity/ sodicity gradient is allotted to each genotype. Further, irrigation with saline waters of predetermined composition is also practiced to establish desired soil salinity levels particularly when relative sensitivity of different growth stages are sought to be compared.
The genotypes with good germination rates has shown a reduction in fresh and dry weight in the vegetable phase under salt stress than in poorly developed ones. Therefore, salt tolerance trials throughout the life cycle or in areas where salt is most sensitive, will be required to compare salt tolerance in different lines [16]. Methods of artificial salt stress, such as slow compression and shock of salt, can lead to results different from those of field testing [17]. The enforcement of salt stress by the gradual exposure to NaCl instead of salt shock has been recommended in genetic and molecular studies because it reflects natural phenomena of salt stress. However, the ideal type of gradual salt impose is technically difficult [18, 19]. Researchers are looking for a simpler or more accurate approach to predicting salt tolerance so that they can better select tolerant plant species or tolerant genotypes. The ability to accumulate photosynthates, proline and glycine-betaine, as well as ion precipitation can be used as a means of biochemical or physiological selection for salt tolerance in canola [20, 21]. The accumulation pattern for various salt overly sensitive (SOS) transcripts after 24 hours of salt stress in various cultivars showed a strong positive association with salt tolerance among Brassica species [22]. Cell membrane stiffness associated with antioxidant enzyme activities (superoxide dismutase, catalase and peroxidase) can be particularly effective in identifying canola with high salt tolerance. To date, no uniform index has been used to test salt tolerance [23].
Breeding salt tolerance in crop plants is considered one of the ways to combat the global problem of increasing soil salinity in agricultural land. Stresses under adverse soil conditions are very complex and are often associated with climate hazards. The salt stress varies from place to place even during the season. Soil salinity is often associated with unhealthy nutrient inequalities (deficiencies/toxins) and other problems and plants adapted different types of strategies to overcome on it (Figure 3).
Problems due to Salt stress and combating strategies in plants.
The interaction between soil salinity and other environmental factors influences the plant’s response to that salt stress. Such problems are due to the slow evolution of plant species that thrive in adverse edaphic areas [24]. Therefore, it is necessary that the genetic material of plants should be tested in targeted areas with sufficient salt stress to find reliable sources of tolerance. Developing crop varieties with increased salt tolerance are considered to be the most promising, energy-saving and economical method than major engineering processes and soil rehabilitation techniques that have exceeded the limits of smallholder farmers [25].
Exploration of the heritable potential of a certain trait within the existing germplasm for a given crop would provide information on factors such as salt tolerance for plant breeders. The both additive and non-additive gene actions involved of in the inheritance of characteristics. High narrow-sense heritability estimates were observed for Ca2+, K+, Na+, K+/Na+, Ca2+/Na+ and stress tolerance index, indicating the prime importance of additive effects in their genetic control [26]. Higher estimates of GCV, PCV, heritability and genetic advance (% of mean) under saline condition was observed for main shoot length, number of pods on main shoot and yield per plot, indicated that these characters might be controlled by additive genes [27, 28]. Salt tolerance was mainly controlled by dominant genes with an additive effect. The dominant effect played a major role and over-dominance might have existed in salt tolerance [29, 30]. The traits like main shoot length, number of pods on main shoot and yield per plot could be improved effectively by selection as these might be controlled by additive genes. Indian mustard, which was thought to be the moderately salt-tolerant species, also showed a decrease in shoot length and root length, electrolyte leakage, protein content, K+/Na+ ratio due to differential regulation of Na+ in root and main stem by inhibition of entry from roots to shoot and retain higher photosynthetic characteristics than other species [10]. The fencing of selection processes should therefore be based on such indicators as a priority in the development of the most productive varieties of Indian mustard for saline condition.
In an effective breeding program, the discovery of a large variety of potential variants in a plant’s genetic pool is a prerequisite; such genepools are needed to provide the required genetic diversity. Genetic diversity provides parental material from well-adapted landraces to enhance local adaptation. It helps to overcome the tendency to find a problem in the soil and provides a basis for fulfilling the needs of the novels. The conventional methods of improving plant salt tolerance generally employ selection for seed yield and there are few examples of producing salt tolerant varieties following these approaches at ICAR-CSSRI. These varieties are extremely popular with the farmers and their certified seeds are in great demand. The areas under their cultivation is fast expanding and increasing every year. The adoption of these varieties by the farmers has helped in great deal to enhance their economic status.
Using this methods of breeding researchers at the ICAR-Central Soil Salinity Research Institute (ICAR-CSSRI), Karnal has developed five cultivars of salt-tolerant Indian Mustard (
Parameter/Variety | CS 52 | CS 54 | CS 56 | CS 58 | CS 60 |
---|---|---|---|---|---|
Year of development | 1997 | 2005 | 2008 | 2017 | 2018 |
Plant height (cm) | 170–175 | 160–170 | 198–202 | 180–185 | 182–187 |
Maturity duration (days) | 130–135 | 121–125 | 132–135 | 130–135 | 125–132 |
Seed type | Medium | Bold | Medium | Bold | Bold |
1000-seed weight (g) | 4.5–5.0 | 5.0–5.5 | 4.5–5.0 | 5.0–5.5 | 5.0–5.2 |
Salinity tolerance (ECe dS/m) | 6–9 | 6–9 | 6–9 | 6–11 | 6–12 |
Sodicity tolerance ( | 8.5–9.3 | 8.5–9.3 | 8.5–9.3 | 8.5–9.4 | 8.5–9.5 |
Yield in non stress(t/ha) | 1.8–2.0 | 2.0–2.4 | 2.2–2.6 | 2.6–2.8 | 2.5–2.9 |
Yield in salt stress(t/ha) | 1.5–1.6 | 1.6–1.9 | 1.6–1.9 | 2.0–2.2 | 2.0–2.2 |
Oil Content | 37–38% | 38–39% | 38–39% | 39–40% | 40–41% |
Time of sowing | Upto 15th October | Upto 15th October | Upto 15th November | Upto 25th October | Upto 25th October |
Recommended ecology | Salt affected Areas |
Salinity tolerant cultivars of Brassica species developed through conventional breeding.
In this method, space planting of F1 was done and harvested in bulk, while the planting of F2 to F6 generations done at commercial seed rate and spacing and harvested in bulk (Figure 4). The size of population in each generation was about 30,000 plants. These were space planted in the F7 generation, and, only 5000 plants with desired characters confers to salt tolerance under salinity (ECe 12.0 dS/m) and sodicity (pH 9) conditions were selected. Seeds of these selected plants were separately harvested. Individual plant progenies were grown in multi-row plots. Weak and inferior progenies were rejected and only 300 individual homozygous plant progenies with desirable traits were selected and harvested in bulk. A preliminary yield trial was conducted for two years for agronomic traits and resistance/tolerance to disease and mustard aphid infestation, along with the national check varieties. Replicated yield trials were conducted for three years under saline and alkaline conditions in salt-affected soils [30].
Development of salt tolerant Indian mustard variety CS 60 (a) Bulk Method; (b) Genotype CS 60 under saline field (ECe 15 dS/m).
If genetic diversity is fully utilized by continuous selection, then diversity may be sought through alternatives such as chemical and radiation, protoplast fusion, or recombinant DNA techniques. Different laboratories are undertaking studies on elucidating salt tolerance mechanisms following molecular and biotechnological approaches. Efforts for the sequencing of
More recently, research into salt tolerance in plants has shifted from genetic mapping to molecular characterization of salt responsive genes. Increased understanding of biochemical pathways and mechanisms that involved in plant stress response has made it clear that many of these methods are common defense mechanisms that can be used by salt, drought and cold, although sometimes alternatives signaling pathways may be used. The molecular mechanism of salt tolerance expressed in model plants will facilitate the identification of target genes and the development of transgenic salt-tolerant plants in Brassica plants (Figure 5). Overexpression of antiporters (SOS1, SOS2, SOS3, ENH and NHX) as well as antioxidant genes (MPK1, DHAR3, APX1, APX4 and MDHAR6) in mustard play an important role in reducing the effects of salt and enhance salt tolerance [10].
The existence of a more efficient salt scavenging system composed of ionic module (SOS1, SOS2, SOS3, ENH and NHX) and oxidative module (MPK1, DHAR3, APX1, APX4 and MDHAR6) in the salt tolerant mustard.
The SOS pathway consists of the plasma membrane Na+/H+ antiporter SOS1, the protein kinase SOS2, and the Ca2+ binding protein SOS3. An increase of Na+ concentration elevate the intracellular Ca2+, and SOS3 binds Ca2+ and activates SOS2 to form a compound that phosphorylates membrane-derived plasma SOS1. Finally, over-expression of SOS1 leads to Na+ efflux overhead [31]. In addition, AtHKT1 is involved in the recirculation of Na+ from shoots to roots, possibly by promoting Na+ movement into phloems in shoots and translocation into roots. The role of AtNHX1 in salt tolerance through increased Na+ compartmentation in the vacuoles [32, 33, 34, 35]. SOS1 and SOS3 are constitutively expressed in Brassica plants, while the pattern of SOS2 expression amongst
Transgenic
The QTL mapping is the best way to identify the underlying genes, though it is difficult and time-consuming. Creating an association map, which uses the highest number of historical recombination events/relics that occur throughout the evolutionary process of mapping population, enables genetic engineering in small genomic regions [40]. Exciting results have been obtained from independent studies on salt tolerance in the Brassicaceae, particularly in Arabidopsis. Most of the identified QTLs that control salt tolerance were different from each other, because the difference in mapping populations and the features under investigation. Normal QTL for germination percentage was detected at 20 cM in chromosome 1 associated with the RAS1 gene, a poor salt-tolerant controller during seed germination and early growth [41]. Another QTL found at 50 cM in chromosome 4 of the candidate AT4G19030 gene [42], whose level of expression reduced by ABA and NaCl [43]. These results suggest a complex genetic network regulating salt tolerance with differential genetic determinants in different accessions. Other QTLs of various traits are embedded: for example, salt responses and root-length QTLs on chromosomes 1 and 3, indicating that these two loci may contain gene-regulating salt tolerance expressed by root growth. However, genome-wide association studies with larger samples are considered to be more reliable and highly productive.
However, studies on QTLs or genes that regulate salt tolerance in Brassica plants are still very limited. To date, the practice of breeding salt tolerance in Brassica has been unsuccessful due to the unavailability of the polymorphic and cross transferability markers and highly salt sensitive lines. Concerns have resulted in a comprehensive breeding program for the development of high-yielding salt-tolerant mustard at the ICAR-Central Soil Salinity Research Institute (ICAR-CSSRI), Karnal and also leading to the changing salt tolerance paths of Brassica juncea by mutation results in the development of highly salt sensitive mutant CS 614-1-1-100-13 and CS 245-2-80-7 that are being used in recombinant inbred lines for mapping of QTLs. Researchers and farmers are trying to understand the salt-tolerance mechanisms and the screen for stable salt-tolerant genotypes to be used in the breeding programs. Efforts have also been made to develop salt-tolerant Brassica transgenic plants with a gene-specific role in ion homeostasis and osmolyte accumulation [44].
Based on our findings on we have developed a model for the salt tolerance mechanism in Indian mustard (Figure 6) and conditioning the differential functions of antiporter and antioxidant transcripts in the mitigation of detrimental effect of salt stress [45]. Model suggested the three-way effect of salt stress on mustard plants; (i) Decreasing stomatal conductance results in the decreased intercellular CO2 which caused diminishing activities of photosynthetic enzymatic machinery and decline in net photosynthesis rate. (ii) Production of reactive oxygen species (ROS) which disrupt the membrane system and limited the carboxylation process results in the least photosynthesis. (iii) Imbalance in the cellular ionic concentrations due to increased uptake of Na+ and decreased K uptake which caused ion toxicity. This ion toxicity leads to decrease in leaf area and early leaf fall down and limited carboxylation results in declined photosynthesis rate. The salt tolerant mustard genotypes counteract on these toxic paths by activation of antioxidant gene network for ROS scavenging and antiporter gene complex that enhanced sequestration of Na+ in roots and reduced toxic Na+ transport to shoots, hence, makes mustard plant tolerant to salt stress.
A predicted model for the salt tolerance mechanism in Indian mustard.
Modern agriculture certainly requires commercial crops that tolerate salt for the purpose of crop trade. Genetic adaptation of crops to salinity requires that sufficient heritable variability exists within species to permit selection of salt tolerant strains and that those plant characteristics that confer salt tolerance be identified. Modern varieties have a relatively narrow genetic base and are poorly adapted to adverse environments such as salinity. However, endemic genotypes from problem environments may provide the basic germplasm for breeding salt tolerant varieties with acceptable yield potentials. Notwithstanding, the, genetic variations for salt tolerance among agricultural crops are very less, because most of the cultivated genotypes have been selected from normal environment where salt tolerant traits must have been gradually discarded, however variability for salt tolerance are similar in many wild progenitors due to where natural selection in response to salty habitats. Recent in-depth studies have identified various pathways at physiological and cell levels in which wild plants respond to salt stress. Due to the close relationship and significant variability between and within the Brassica species show great potential for breeding salt tolerance in Brassica plants. However, it is clear that to connect the salt tolerance factor and the QTL site to the chromosome, a proper breeding system assisted by markers is a prerequisite.
All the authors declare that they have no conflict of interest.
Photodetectors are devices that sense the light and convert it into an electric current. Photodetectors are essential components of many devices that are a part of our day to day life [1, 2, 3, 4, 5]. Primarily, silicon (Si) has been a material of choice for photodetector applications. Such photodetectors are readily integrated with complementary metal oxide semiconductor (CMOS) technology. The aggressive scaling has reduced the cost of Si-based devices and expanded their range of applications. Though Si photodetectors have evolved and developed over the years. But their performance is limited by the indirect nature of the bandgap of Si. The absorption of Si is limited to the visible and near-infrared parts of the electromagnetic spectrum. Also, the indirect nature of Si′s bandgap leads to phonon generation to conserve the momentum during the light assisted transition of carriers from lower energy to higher energy. These phonons lead to scattering of the carriers and thereby reduce the efficiency of Si photodetectors. Also, Si as a material is not a good absorber of light in bulk form, further degrading Si photodetectors’ efficiency. These limitations of Si photodetectors have prompted a quest in the research community for alternate materials. Two dimensional (2D) materials, among the class of novel materials for optoelectronic applications, have shown favorable characteristics. Features like direct nature and wide range of bandgap, atomically thin nature, efficient light-matter interaction, and heterostructures forming are interesting. The class of 2D materials encompasses materials like graphene, transition metal-di-chalcogenides (TMDCs), Xenes etc. 2d materials are artificially derived materials. These materials are derived from layered van der Waals solids. In van der Waals solids, the atomic arrangement is such that the constituent atoms are held together by covalent or ionic bonds giving rise to atomic layers, whereas these atomic layers are held together by van der Waals interactions. The weak nature of van der Waals forces makes it possible to cleave individual layers from these materials. It is possible to obtain a free-standing single atomic or few atomic layers via mechanical exfoliation [6, 7] or liquid phase exfoliation [8, 9]. Graphene, which is a single layer of carbon atoms arranged in a hexagonal manner, is regarded as the original 2D material. Over the years, it has been revealed that graphene possesses many appealing electronic, mechanical, optical and thermal properties. [10, 11, 12]. Interaction of light with graphene occurs over a broad bandwidth range (terahertz to ultraviolet wavelengths) because of semi-metallic/gapless nature. This makes graphene a candidate for wide spectral range photodetectors. The atomically thin nature of graphene limits its absorption coefficient [13, 14, 15]. Graphene absorbs only 2.3% of incident light (visible and ultraviolet), making this a primary limitation of graphene for photodetector applications. A high absorption coefficient is desirable for an optimum magnitude of photocurrent [16, 17, 18]. For the efficient operation of a photodetector, a longer lifetime of the photo exited carriers is desired. Graphene’s gapless nature results in a shortened lifetime of photo-excited carriers, which further limits graphene photodetectors’ performance. Beyond graphene, TMDCs have also attracted a lot of attention for optoelectronic applications over the past decade. One advantage of TMDCs over graphene is their semiconducting nature. TMDCs possess varied bandgaps, thus making them applicable for broadband photodetection. TMDCs can be represented by the general formula of MX2, where M represents a transition metal and X represents a chalcogenide atom. The arrangement of atoms in MX2 is such that the metal atom is sandwiched between the two chalcogenide atoms, as shown in Figure 1. TMDCs detect light at different wavelengths because of layer dependent bandgap [19, 20, 21]. Most of the TMDCs have a direct nature of the bandgap, limiting the phonon scattering in TMDCs photodetectors, which leads to better efficiency [22]. 2D materials have localized electronic bands, leading to sharp peaks in the density of states (DOS) called Van Hove singularities at specific energies [22]. Generally, in 2D materials like TMDCs, these singularities reside near conduction and valence bands. This leads to an increased probability of electron–hole pair generation upon excitation with light [22, 23]. TMDCs photodetectors show excellent light to current conversion with high responsivity [22]. Although TMDCs based photodetectors have shown an appealing development in their performance over the years, these devices are limited by slow response speed. Furthermore, TMDCs photodetectors are still behind the absorption efficiency of bulk Si photodetectors. Apart from these 2D materials, materials like silicene, phosphorene etc., have shown promising theoretical results as far as optoelectronic applications are considered.
Structural arrangement of TMDCs (MoS2). (a) Top view and (b) side view. Cyan and Yellow balls are Molybdenum and Sulfur atoms respectively.
Though the field of 2D materials is still developing, the early results of optoelectronic devices based on these materials are very promising. The unique properties of 2D materials have ushered in a lot of theoretical and experimental research for optoelectronic applications over the past decade or so. This has led to the proposal of numerous photodetectors based on 2D materials both theoretically and experimentally. This chapter aims at presenting an insight into the novel photodetectors based on 2D materials. Section 2 offers a discussion on photodetectionchanisms in 2D materials. Section 3 presents a discussion on photodetectors based on 2D materials and their heterostructures; Section 4 presents a brief summary of the chapter and future scope of 2D materials for photodetector applications.
Generally, photocurrent generation mechanisms are divided into three categories, viz. photovoltaic effect, photo-thermoelectric effect, and photo-bolometric effect. In the photovoltaic effect, a built-in electric field results in the separation of the electrons and holes. This built-in electric field may be generated due to a Schottky barrier at the metal–semiconductor interface. Photodetectors working under this mechanism are called photodiodes. In the photo-thermoelectric effect, a non-uniform light source is used. This light source leads to non-uniform heating of the channel, resulting in a temperature gradient within the channel. Due to this temperature gradient, carriers move from the high-temperature region to the low-temperature region. The migration of the carriers leads to their accumulation in the low-temperature region, which results in a potential. The photo-bolometric effect is based on uniform heating of the material under illumination. This uniform heating results in a change in the resistivity of the material. This effect is directly proportional to the variation of the material’s conductivity and the increment in temperature caused by light irradiation. In contrast to the photo-thermoelectric effect, the photo-bolometric effect does not drive the current but only changes the intensity of the current under external bias and illumination.Another unique mechanism observed in optoelectronic devices like photodetectors is internal photoemission (IPE). IPE involves photoinjection of electrons from an emitter/source (metal or semiconductor) into the conduction band of a collector/drain (semiconductor or insulator) in a BJT/FET. The holes are photoinjected into the valence band of the collector/drain and is called as hole photoemission [24]. In IPE, an optical excitation of electrons in the metal to an energy above the Schottky barrier is involved. These excited electrons are then transported to the conduction band of the semiconductor. The Initial theory of IPE was proposed by Fowler [25, 26]. However, this theory does not take the thickness of the Schottky metal layer into consideration. Over the years the original theory of IPE has been refined largely resulting in much better assessment of the performance of the devices based on this effect [27, 28].
Graphene is regarded as the original 2D material and has a hexagonal arrangement of atoms. Graphene has a planar geometry contrary to some other 2D materials like Xenes (silicene, germanene stanene etc.). The Xenes, in general, have a buckled geometry wherein the two sub lattices of the hexagonal lattice are slightly displaced with respect to each other. Graphene can absorb light with a wavelength ranging from ultraviolet to mid-infrared [29, 30]. Graphene has small optical absorption due to its atomically thin nature, limiting the photoresponsivity of the photodetectors based on it. A graphene photodetector exhibited a bandwidth of 500 GHz and a photoresponsivity of 0.5 mAW−1 [31]. A metal-graphene-metal (MGM) photodetector having asymmetric electrodes has been investigated for extended operating frequency. This device shows an external photoresponsivity of 6.1 mAW−1.
Some of the essential advantages of graphene photodetectors are high speed, ultra-broadband frequency range, and compatibility to circuits [32]. Compared to conventional semiconductors, graphene photodetectors show low photoresponsivity, which proves to be a significant drawback of such photodetectors. To overcome this and the other drawbacks, some techniques have been proposed to improve graphene photodetectors’ optical absorption. For example, the use of nanostructured plasmonics leads to enhanced light concentration in the device via plasmonics resonance [33, 34]. This helps in improving the local electric field [33, 34]. Apart from enhancing the quantum efficiency, the plasmonics can also help in achieving multicolor detection [35]. A graphene photodetector possessing plasmonics nano-antennas sandwiched between two graphene layers shows a quantum efficiency of up to 20%. Though this method may offer quantum efficiency improvements, it reduces the device’s operational bandwidth as the nanostructures’ resonance determines the working wavelength in these systems.
Another method to improve graphene photodetectors’ photoresponsivity is to integrate quantum dots with graphene [36]. The photoresponsivity and photodetection gain of such a device are 107 AW−1 and 108, respectively. The presence of quantum dots in this device helps the photo-excited carriers (electrons or holes) to reach the graphene sheet while trapping the opposite type of carriers (holes or electrons). This leads to a phenomenon known as field-effect doping. Graphene photodetectors using PbS quantum dots have also been fabricated [37]. The device portrays a photoresponsivity of 107 AW−1. Graphene-quantum dot photodetectors are limited by factors like low operational speed and low operating bandwidth.
Another method to improve the photoresponse in graphene photodetectors is to use micro-cavities [38, 39, 40, 41, 42]. Such photodetectors are characterized by high speed, high efficiency, ultra-wide bandwidth and high photoresponsivity. The disadvantage of using micro-cavities is that the device’s dimensions are relatively large compared to traditional photodetectors [41].
MoS2 in its monolayer form has exciting properties like high carrier mobility 200 cm2V−1 s−1 [8, 43, 44], direct bandgap of ≈1.8 eV [43, 45], high On/Off ratio of current [45], strong light-matter interaction [8, 44], mechanical flexibility, chemical stability and ease of processing etc. Such exciting features of MoS2 in its monolayer and few-layer forms make it the most widely studied 2D semiconductor for optoelectronic applications. A photodetector having a typical field-effect transistor (FET) configuration was first reported by Yin et al. [46]. The device comprises of a mechanically exfoliated monolayer of MoS2 monolayer nanosheet as the effective region. The device shows a unique response with a cut-off wavelength of 670 nm. The cut-off wavelength is consistent with the bandgap of MoS2 in its monolayer form (1.8 eV). The maximum responsivity of this device is 7.5 mAW−1 along with a response speed of 50 ms. A similar photodetector/phototransistor was reported by Lopez-Sanchez et al. [47]. Again, this device is based on an exfoliated MoS2 monolayer but has an improved responsivity of 800 mAW−1 and a cut-off wavelength of 680 nm [47]. The model of the device is shown in Figure 2. The improvement in the device performance is attributed to improved mobility of the carriers, quality of the contacts and positioning technique. Apart from improved responsivity, the device portrays a low noise equivalent power (NEP) of 1.5 × 10−15 WHz−1/2. Such a low value of NEP is associated with a low value of dark current.
Model of the exfoliated single layer MoS2 phototransistor [
Furthermore, the dark current in this device is limited by the bandgap of MoS2, which reduces the role of thermally excited carriers. However, the device is relatively slow in its response time, which is of the order of several seconds. Though the response time can be reduced (to 0.6 s) by using short pulses on the gate terminal to remove trapped charges, the response time is still considerable compared to other devices [46]. The photodetector reported by Lopez-Sanchez et al. shows a sub-linear dependence of photocurrent on the intensity of the light. Such behavior and the surrounding dependent response speed of MoS2 indicate that charge trapping in MoS2 and/or at the MoS2-SiO2 interface plays a vital role in the sensing process.
Some of the properties and qualities of MoS2 depend on the number of layers; accordingly, the performance of the photodetectors varies with the number of layers of MoS2 [43, 45, 48]. For example, in bulk form, MoS2 is an indirect bandgap semiconductor and is not suitable for optoelectronic applications, whereas, in its monolayer form, it is a direct bandgap semiconductor, making it suitable for optoelectronic applications. The lifetime of the photoexcited carriers is also dependent on the number of layers. Lee et al. have fabricated phototransistors, having single, double and triple layer MoS2 as the effective region. The optical bandgap of monolayer MoS2 is 1.82 eV, whereas, for double and triple layer MoS2, it is 1.65 eV and 1.35 eV, respectively. Based on the observations, it is seen that triple layer MoS2 photodetector shows good detection for the red light, whereas double and monolayer MoS2 photodetectors show good detection for the green light. The layer dependent bandgap in MoS2 allows for its use in wavelength range up to near-infrared (NIR) [49]. Multilayer MoS2phototransistors show a degraded responsivity value of 100 mAW−1. Khan et al. have also demonstrated that parameters like responsivity and response speed show a high dependence on the number of MoS2 layers [50].
The properties of 2D MoS2 are distinctly dependent on the method of preparation. Zheng et al. reported a phototransistor based on chemical vapor deposition (CVD) grown MoS2 [51]. This device has a maximum responsivity of 2200 AW−1 in vacuum operating at a wavelength of 532 nm. The same device shows a responsivity of 780 AW−1 in air. The cause for such a decrease in responsivity is the adsorbates. Due to the large surface-to-volume ratio of MoS2, many adsorbates migrate from ambient air to the surface of MoS2 and the MoS2/substrate interface. These adsorbents act as p-type dopants, leading to carrier scattering and degraded carrier mobility and responsivity in air. The photoresponse could also get affected (decreased) as the adsorbents may act as recombination centers for photoexcited carriers [52].
Perea-Lopez et al. have also fabricated a photodetector based on CVD-grown MoS2 monolayer [53]. The reported device shows a relatively lower responsivity of 1.1 mAW−1 at an illuminating wavelength of 514.5 nm [53]. Such a considerable variation in the two devices’ responsivity shows the significant role of contact resistance in these devices. Another study has put CVD-grown few-layer MoS2 to use for a photodetector [54]. The performance of the device has been evaluated under harsh conditions with a wavelength of 532 nm [54]. Even at 200°C, the device portrays a photocurrent to dark current ratio of 10. Photodetectors based on MoS2 employing other methods of synthesis like liquid exfoliation [55], solution synthesis [56] and magnetron sputtering [57] have also been reported. As compared to mechanically exfoliated and CVD grown MoS2 based devices, these devices show degraded values of responsivities.
In photodetectors, based on monolayer and bilayer MoS2, both photoconductive and photogating effects were observed to contribute to the photocurrent [58]. Different response times were observed for the two effects, respectively, making it possible to identify their independent contribution to the photocurrent. The photogating effect shows an obvious dependence on the gate voltage and is a slow process. The slowness of this effect comes from the longer lifetime of the trapped charges at the MoS2-SiO2 interface. In contrast, the photoconductive effect has a negligible dependence on the gate voltage and is a fast process. The fast response of the photoconductive effect arises from the mid-gap states due to structural defects in MoS2. The photoconductive response can be studied independently by varying the illuminating light faster than the photo-gating effect.
In view of the average performance of MoS2 photodetectors, several techniques have been proposed to improve their performance [59, 60, 61, 62, 63, 64, 65, 66]. One such technique proposed by Leu et al. involves micro-patterning and localized modification of the MoS2 layer [59]. The device is operated at an illuminating wavelength of 532 nm. The local modification is achieved by surface oxidation and oxygen doping. A photodetector based on such a modified MoS2 layer shows improved photoresponse with a responsivity increase of several folds [59]. Kwon et al. proposed a photodetector based on multilayer MoS2 with a bottom gate configuration [60]. As compared to previously reported global gate counterparts, the device shows much-improved photocurrent [49, 60, 67]. The purpose of a bottom gate in such a device is to impose a large tunnel barrier at ungated channel regions, which helps accumulate holes, thereby reducing the potential barrier for free electrons. Once the potential barrier is reduced, there is an increase in the electron depletion region’s thermionic current. Furthermore, photocurrent improvement in the accumulation region arises due to decreased tunnel barrier for photoexcited holes. Also, the dark current is suppressed because of the series resistance from ungated areas. Consequently, the responsivity shows huge improvements and attains a value of 342.6AW−1. Kufer et al. fabricated a MoS2 photodetector, wherein HfO2 encapsulates the MoS2 layer. Upon encapsulation, it was seen that the electronic and optoelectronic properties of multilayer MoS2 photodetector improved [61]. The encapsulated MoS2, along with negligible hysteresis in the transfer characteristics, showed an enhanced n-type behavior. Encapsulation decreases the number of surface adsorbents, which eventually leads to improved performance. Encapsulation results in an increase in the mobility of carriers and a decrease in the contact resistance. These two effects, in combination, give rise to an increased response speed and responsivity. The device’s responsivity can be tuned by the gate voltage and ranges from 10 to 104 AW−1.
Apart from MoS2, other TMDCs have been utilized for photodetector applications. These include MoSe2, WS2, WSe2, MoTe2, ReS2 and ReSe2. This section presents photodetectors based on these materials.
Like MoS2, monolayer MoSe2 has several alluring properties, such as a direct bandgap of 1.5 eV [68], enhanced photoluminescence (PL) [69] and considerable binding energy of excitons [70]. Improvements in the synthesis of MoSe2 via mechanical exfoliation [71, 72] and CVD methods [73, 74, 75] have widened their scope of photodetector applications. Chang et al. and Xi et al. have reported monolayer MoSe2 phototransistors [76, 77]. MoSe2 monolayers for the phototransistors were prepared via CVD methods. The responsivities of the phototransistors are of the order of mAW−1, which is lower than the CVD-grown MoS2 monolayer counterparts by a few orders [51]. However, if the density of the charge impurities and defects are reduced, an improved photoresponse of the order of tens of milliseconds is expected. The responsivity of MoSe2 based devices can be improved by using a CVD-grown multilayer MoSe2 [78]. But the improvement comes at the cost of degraded response speed [78]. A phototransistor based on a few-layer MoSe2 has been fabricated by Abderrehmane et al. [72]. MoSe2 layers were obtained by mechanical exfoliation methods [72]. This device has a response time of tens of milliseconds and a responsivity of 97.1 AW−1 operating at a wavelength of 532 nm.
Photodetectors based on monolayer and few-layer WS2 obtained via different synthesis methods have been reported [79, 80]. The photoresponse of CVD-grown few-layer WS2 has been studied by Parea-Lopez et al. [81]. The photoresponse reportedly shows a high dependence on photon energy [81]. The responsivity and response speed of the device are reported to be 92 μAW−1 and 5 ms, respectively at a wavelength of 457-647 nm. The dependence of multilayer WS2 devices’ responsivity was observed to depend on the surrounding gaseous environment by Huo et al. [82]. The responsivity shows an increase when the environment changes from vacuum (tens of AW−1) to NH3 (884 AW−1) at a wavelength of 633 nm. The increased responsivity is a consequence of the charge transfer between the NH3 gas molecule and WS2. The doping level of WS2 gets modified by the charge transfer, which eventually increases the lifetime of photoexcited carriers and hence the responsivity. Another study conducted by Lan et al. showed a similar surrounding dependent performance of WS2 devices [83]. The device showed a decrease in its responsivity from 18.8 mAW−1 in vacuum to 0.2 μAW−1 in air.
Monolayer and few-layer WSe2 has also been studied for photodetector applications. Zheng et al. have fabricated photodetectors using CVD-grown WSe2 monolayer [84]. The effect of metal contacts having different work functions on the device’s photoresponse is studied [84]. The device exhibits the maximum (1.8 × 10 5 AW−1) and minimum responsivity with Pd and Ti contacts at a wavelength of 650 nm. However, the device with Ti contacts shows a much smaller response time (23 ms) than the device with Pt contacts. The variation in the device’s performance results from the considerable difference in Schottky barriers between WSe2 and different materials, highlighting the significant role of metal contacts in these devices. Pradhan et al. have demonstrated a photodetector based on a trilayer WSe2 [85]. The device exhibits the responsivity and response speed of 7AW−1 and 10 μs, respectively at an illuminating wavelength of 532 nm. Other reports involving graphene contacts and doping of a few-layer WSe2 have been observed to improve the performance of WSe2 photodetectors [66, 86, 87].
A newly introduced 2D material, MoTe2 has excellent electronic and optoelectronic properties, due to which it has received a lot of attention recently [88, 89, 90]. Yin et al. have reported a phototransistor based on exfoliated few-layer MoTe2 [91]. A study of the effect of different metal contacts on the electrical properties of the MoTe2 phototransistor is presented. The device attains a responsivity of 2.56 × 103 under optimum conditions under an illumination of 473 nm laser.
Re-dichalcogenides are different from the majority of other layered TMDCs due to their high crystal symmetry. ReS2 and ReSe2, in their distorted 1 T in-plane structure are anisotropic semiconductors [92]. The electrical, mechanical, and optical properties of these materials are extremely anisotropic, rendering these materials interesting for optoelectronic and electronic applications. The bandgap and carrier mobility of ReSe2 was found to be dependent on the layer thickness by Yang et al. [93]. This allows modification of the electronic and optoelectronic properties of ReS2 devices. A monolayer ReSe2 phototransistor has an exceptional photoresponse with responsivity and response time of 95 AW−1 and tens of milliseconds, respectively [93]. The operating wavelength for the device is chosen to be 633 nm. Just like MoS2 and WS2 devices, the photoresponse of ReSe2 devices is also found to be dependent on the surroundings [50, 51, 82, 83, 94]. The charge transfer between the surrounding gas and ReSe2 consequently affects the device performance. This charge transfer alters the doping in ReSe2 along with the carrier lifetime [94]. One way to avoid this dependence of performance on surroundings is to use encapsulation or passivation. Though the ReSe2 photodetectors/phototransistors show promising results but an obvious disadvantage of these devices is that the current after removing the illuminating light can not return to dark current levels. This disadvantage is a consequence of the slow recombination rate of the photoexcited carriers. However, this issue may be solved by applying short pulses at the gate terminal to reset the device [36].
Because of the anisotropic crystal structure, ReS2, in particular, can be utilized to detect polarized light [95]. The model of one such photodetector is shown in Figure 3. The responsivity of ReS2 photodetectors can be largely improved up to the levels of 3.97 × 103 to 1.18 × 106 by electron doping [96] under illumiation of a 1064 nm laser. Besides improved responsivity, the device portrays a broad range of wavelength detection and fast response speed of the order of tens of milliseconds. Significant enhancement in both the electronic and optoelectronic properties of ReS2 via O2 plasma treatment was observed by Shin et al. [97]. The device exhibits a high responsivity of 2.5 × 107 AW−1 at a laser illumination of 405 nm, which is the highest obtained for a 2D semiconductor based back gated photodetector. Such a high responsivity is a consequence of large thickness (30 nm) and direct bandgap of ReS2 layers. The response time is observed to be inversely proportional to the plasma treatment duration. Prolonged plasma treatment leads to the formation of trap states within the bandgap of ReS2. Such trap states result in enhanced recombination rates of photoexcited carriers, which consequently reduce the response time.
Model of ReS2 photodetector [
In summary, TMDCs photodetectors/phototransistors show a widely varying performance. Responsivities and the response times range from 10−7 AW−1 to 107and 10−5 to 103, respectively. Generally, trap states affect the performance of TMDCs photodetectors. An increase in responsivities is observed at the existence of the trap states in TMDCs and/or at TMDC-dielectric interfaces. However, the response speed is found to decrease because of these trap states. Other factors that affect the TMDCs photodetectors/phototransistors are synthesis methods, number of layers, contact resistance and surrounding environment.
Phosphorous, in its elemental nature, can exist in many forms. One such form of phosphorous is called black phosphorous (BP). With a formation energy of −395 KJmol−1− black phosphorous is a thermodynamically stable form of phosphorous at room temperature. Black phosphorous is similar to graphite in its appearance, properties and structure. Black phosphorous sheets have a puckered geometry [98]. Black phosphorous was first successfully exfoliated in 2014 and has received a lot of attention since then [99, 100]. In its monolayer form, the phosphorous atoms form covalent bonds with three adjacent atoms, which results in a wrinkled honeycomb structure. The corresponding layers are held together by van der Waals forces [101]. Unlike graphene, black phosphorous is a semiconductor with a direct bandgap. Due to its strong anisotropic interaction with electrons and photons, black phosphorous is a strong candidate for electronic and optoelectronic applications.
The bandgap’s direct nature in black phosphorous makes it easy for the carriers to transit to excited states, as there are negligible chances of phonon scattering [102]. The photoelectric characteristics of a black phosphorous FET were studied by Buscema et al. [103]. Figure 4 shows the model of the device. The device operates at a wavelength ranging from visble to NIR part of the spectrum. The device shows an On/Off ratio of 10 along with an electron mobility of 0.5 cm2V−1 s−1. Wavelength ranging from visible to NIR results in a photocurrent generation in the proposed device. The responsivity exhibits a typical increase with a decreasing wavelength and attains a maximum value of 4.8 mAW−1. Chen et al. used a sandwich of hBN-BP-hBN to demonstrate a photodetector with a widely tuneable infrared wavelength range [104]. The device shows an absorption of 3% at a wavelength of 3.4 μm, and the absorption of the device was observed to decrease with increasing wavelength. Furthermore, it was observed that the light absorption decreases with an increase in vertical electrical bias. Due to the vertical bias, the bandgap shrinks, giving rise to an increase in carrier concentration. The high carrier concentration results in decreased photo-carrier lifetime and degraded performance of the device. The hBN layer aims to prevent the black phosphorous from oxidation and provide a clean interface.
Model of the few layer black phosphorous photodetector [
One of the primitive methods to improve the performance of TMDC photodetectors is to use doping. Accordingly, Keng et al. demonstrated an n-type and p-type black phosphorous photodetectors [105]. The concentration of the dopants was found to be dependent on the thickness of the black phosphorous layer. The device shows a responsivity of 1.4 × 104 AW−1 for a device with a black phosphorous thickness of 10 nm [105].
Using a transparent substrate opens up the possibility of novel device designs. Miao et al. have fabricated a photodetector based on multilayer black phosphorous on polyimide film substrate [106]. The device shows a responsivity of 53 AW−1. It is observed that when the device is illuminated by infrared light, enhanced scattering of the carriers with the phonons occurs, which eventually degrades the carrier mobility and the performance of the device. However, such behavior is not observed when a SiO2/Si substrate is used instead of polyimide film.
The ever-growing evolution and development of 2D materials have led to the formulation of 2D van der Waals heterostructures. Based on these heterostructures, several photodetectors have been reported recently. Apart from their high degree of integration, these devices exhibit excellent performance. The electronic structure and properties induced between these 2D heterostructures’ layers show promising characteristics as far as electronic and optoelectronic applications are concerned. 2D heterostructures/heterojunctions are essential building blocks of modern electronic devices [107]. The band structures of the constituent 2D materials of these heterostructures undergo considerable changes due to electrostatic interactions. Xue et al. have fabricated a MoS2/WS2 vertical heterostructures based photodetector [108]. Mo, S and WO3 were used to prepare the MoS2/WS2 heterojunction. The device shows a high rectification along with a considerable responsivity of 2.3 AW−1. The characteristics of the device are evaluated at an illuminatring light of 450 nm. The interfacial built-in electric field prompts the separation of the photo-generated carriers [109]. On transferring the heterojunction to the polydimethylsiloxane (PMDS) substrate, a decrease in photocurrent is observed due to trapping states between the heterojunction and the substrate [47]. Duan et al. demonstrated a heterojunction diode based on WSe2/MoS2 heterojunction [110]. The heterojunction was obtained by transferring the exfoliate MoS2 to a physical vapor deposition (PVD) grown WSe2 monolayer. A significant rectification ratio, along with high external quantum efficiency (EQE), was observed at an operating wavelength of 514 nm. It is noteworthy to mention that the EQE of the device is much higher than what is achieved in a lateral doped WSe2 p-n homojunction [111]. Such a behavior is a consequence of the much better charge separation at the vertically stacked junction interface. Peng et al. have also reported a heterojunction between MoS2 and WSe2 [112]. The MoS2/WSe2 heterojunction is obtained by mechanical exfoliation and transfer methods. A high charge transfer of 99% from WSe2 to MoS2 is observed in a very short time of 470 fs [112]. The device shows promising characteristics for sub-picosecond applications.
Apart from the semiconducting materials based heterostructures, graphene has also been utilized for heterostructures formation. Graphene may not be suitable for photodetector applications independently due to its zero bandgap and high light transmittance. Yu et al. formulated a photodetector based on MoTe2/graphene heterostructures [113] as shown in Figure 5. MoTe2 multilayer serves as a light active material in the said heterostructure, and graphene monolayer serves as an efficient transport path for photo-excited carriers. The heterostructure shows better performance as compared to individual graphene and MoTe2 based devices. MoTe2/graphene photodetectors work on the principle of photogating effect. Due to this photogating effect, electrons are trapped in localized states of MoTe2 and holes are shifted towards the graphene layer. The high carrier mobility of graphene allows for a quick extraction of the holes injected into the graphene layer. This results in an enhanced photocurrent in the device. The device shows exceptional values of photoconductive gain and responsivity.
Photodetector based on MoTe2/graphene heterostructure [
Britnell et al. demonstrated a photodetector based on the heterostructures of a few-layer TMDCs and graphene [114]. The device’s performance depends on the encapsulation of one or more layers of TMDC sheets with graphene. The device has a sandwich structure wherein the TMDC photoactive layer is encapsulated between the top and bottom graphene electrodes. Because of the transparency of graphene, the illuminating light can reach efficiently to the TMDC layer. An appreciable photocurrent is observed when the illuminating light impinges on the overlapped regions of graphene and TMDC. The direction of the photocurrent aligns with the direction of the built-in electric field resulting from the gate voltage. This allows to modulate the photocurrent through gate voltage. Due to graphene, the extraction of charges is swift, thus reducing the recombination rate of photo-excited carriers. A similar structure is reported by Duan et al. as well [115]. The device consists of a vertical sandwich of graphene-MoS2-graphene heterojunction. Similar to the device reported by Britnell et al. [114], the top and bottom layers of graphene act as electrodes, whereas the middle MoS2 layer acts as the barrier layer. Upon illuminating the MoS2 layer, the electron–hole pairs get separated asymmetric potentials at the graphene/MoS2 interface, which leads to an appreciable photocurrent [115]. A graphene-WSe2-graphene heterostructure based photodetector is reported by Massicotte et al. [116]. The heterostructure is packaged with hBN layers. The device exhibits an ultra-fast response time of 5.5 ps.
Apart from graphene, another novel material called silicene has received a lot of attention in recent years. Silicene, regarded as the ‘silicon version of graphene,’ also has a hexagonal structure [117, 118, 119]. Silicene is the single-layer version of graphene, having the constituent Si atoms arranged in a hexagonal form via covalent bonds [22, 23]. Silicene shares many properties of graphene, like zero bandgap, high mobility of carriers and the presence of a Dirac cone in its band structure. Apart from these excellent electronic properties, one advantage of silicene over graphene is its expected integration with the present state of the art Si-based technology. Kharadi et al. have proposed a photodetector based on silicene/MoS2heterostructure [22]. The model of the device is shown in Figure 6. Due to the high mobility of carriers in silicene, it is used as a high-velocity transport path for the photo-excited carriers. Illuminating the device’s active region with a light of 650 nm results in the electron–hole pair generation. The electron–hole pairs are separated at the silicene/MoS2 heterostructure interface due to the built-in electric field generated by a combined effect of charge transfer between silicene and MoS2 and the gate voltage. Apart from an appreciable photoconductive gain of 2.5 × 1011, the device exhibits considerable values of responsivity (5.66 × 105 AW−1) and detectivity (4.76 × 1010 Jones).
Model of Si/MoS2 heterostructure based photodetector [
Table 1. presents the characteristics of the optoelectronic devices based on different 2D materials. In general it can be seen that the light sensitive devices based on 2D materials have shown a steady increase in the performance over the years. Depending on the bandgap of the material used, the photosensitive device can be used in different wavelength regions of the electromagnetic spectrum.
Device Type | Wavelength | Responsivity | Response Speed | NEP/Detectivity |
---|---|---|---|---|
Single-Layer MoS2 Phototransistor [46] | 670 nm | 7.5 mAW−1 | 50 ms | — |
Ultra-Sensitive Monolayer MoS2 Photodetector [47] | 680 nm | 800 mAW−1 | 0.6 s | 1.5 × 1015 WHz−1/2 |
High-detectivity multilayer MoS2 phototransistors [49] | Up to NIR | 100 mAW−1 | — | — |
High-gain CVD-grown MoS2 monolayer phototransistor [51] | 532 nm | 2.2 × 103 AW−1 in Vacuum 780 AW−1 in Air | — | — |
High photosensitivity few-layered MoSe2 back-gated field-effect phototransistor [72] | 532 nm | 97.1 AW−1 | ~10 ms | — |
Few Layer WS2 Phototransistor [81] | 457-647 nm | 92 μAW−1 | 5 ms | — |
Multilayer WS2 Nano-flakes Photo responsive FET [82] | 633 nm | 5.7 AW−1 in Vacuum 884 AW−1 in NH3 Environment | < 20 ms | — |
WSe2 Monolayer Phototransistor [84] | 650 nm | 1.8 × 105 AW−1 | < 23 ms | 1014 Jones |
High Photo responsive Few-layered WSe2 Transistor[85] | 532 nm | 7 AW−1 | 10 μs | — |
ReSe2 nanosheet transistor [93] | 633 nm | 95 AW−1 | ~ 10 ms | — |
Few-layer Black Phosphorus FET [103] | Visible-NIR | 48 mAW−1 | — | — |
Silicene/MoS2 heterostructure [22] | 650 nm | 5.66 × 105 AW−1 | — | 4.76 × 1010 Jones |
Characteristics of photodetectors and phototransistors based on different 2D materials.
This chapter has summarized the present advances of the photodetectors based on 2D materials. With the ongoing research on 2D materials and their heterostructures, the class of 2D materials may mature to a large extent as far as electronic applications in general and optoelectronic applications, in particular, are concerned. Despite the promising results, certain gaps need to be bridged for the swift development of 2D material-based devices. First, convenient and cost-effective methods for the synthesis of high-quality 2D materials should be explored and developed. Second, several new properties of 2D materials are yet to be fully explored and understood. An exhaustive effort should be focused on exploring and understanding these properties. Third, more effort should be made to formulate the application-specific heterostructures of 2D materials. The electronic and optoelectronic applications may receive a heavy push upon concurrent improvements in material growth processes and fabrication methods.
The future applications of 2D materials depend on effective integration with the present Si-based technology. Materials like silicene, germanene etc., have brought a fresh breath to 2D materials’ integration with Si-based technology. Though high-performance optoelectronic applications of 2D materials have been realized, there is still a lot of room for improvement. In general, one may not be surprised if wide-spread 2D material based applications are seen in the commercial market in the near future.
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The CC BY 3.0 and CC BY 4.0 license permits Works to be freely shared in any medium or format, as well as the reuse and adaptation of the original contents of Works (e.g. figures and tables created by the Authors), as long as the source Work is cited and its Authors are acknowledged in the following manner:
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\\n"}]'},components:[{type:"htmlEditorComponent",content:'Copyright is the term used to describe the rights related to the publication and distribution of original Works. Most importantly from a publisher's perspective, copyright governs how Authors, publishers and the general public can use, publish, and distribute publications.
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The CC BY 3.0 and CC BY 4.0 license permits Works to be freely shared in any medium or format, as well as the reuse and adaptation of the original contents of Works (e.g. figures and tables created by the Authors), as long as the source Work is cited and its Authors are acknowledged in the following manner:
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Buildings have a significant share in total energy consumed globally; therefore, they have a profound impact upon the environment. Energy is used in every stage of building life cycle (these stages are choice of locality, architectural design, structural systems and material selection, building construction, usage and maintenance, demolition, reuse-regain-recycle, and waste disposal). According to World Watch Institute data, buildings are responsible for the annual consumption of 40% of the world's energy. Energy consumption of buildings can be reduced significantly in every stage of a building life cycle. This study investigated the energy-efficient methods in building life cycle. In this context, we give information about the life cycle of building and explain energy-efficient guiding principles in life cycle stages.",book:{id:"5361",slug:"energy-efficient-buildings",title:"Energy Efficient Buildings",fullTitle:"Energy Efficient Buildings"},signatures:"Izzet Yüksek and Tülay Tikansak Karadayi",authors:[{id:"186397",title:"Dr.",name:"İzzet",middleName:null,surname:"Yüksek",slug:"izzet-yuksek",fullName:"İzzet Yüksek"},{id:"186398",title:"Prof.",name:"Tülay",middleName:null,surname:"Tıkansak Karadayı",slug:"tulay-tikansak-karadayi",fullName:"Tülay Tıkansak Karadayı"},{id:"374197",title:"Dr.",name:"Izzet",middleName:null,surname:"Yüksek",slug:"izzet-yuksek",fullName:"Izzet Yüksek"},{id:"374198",title:"Dr.",name:"Tülay Tikansak",middleName:null,surname:"Karadayi",slug:"tulay-tikansak-karadayi",fullName:"Tülay Tikansak Karadayi"}]},{id:"51988",doi:"10.5772/64902",title:"Energy Efficiency in Manufacturing Facilities: Assessment, Analysis and Implementation",slug:"energy-efficiency-in-manufacturing-facilities-assessment-analysis-and-implementation",totalDownloads:2536,totalCrossrefCites:5,totalDimensionsCites:7,abstract:"Manufacturing facilities are one among the largest consumers of energy. Efforts to improve energy efficiency are an increasing concern for many manufacturing facility engineering managers. This can be achieved by evaluating energy end uses (e.g., lighting, processing equipment, and heating, air conditioning, and ventilation (HVAC) systems), and by implementing measures to reduce the total amount of energy consumed for one or more of the end uses. Throughout the 40 years of its existence, the US Department of Energy’s Industrial Assessment Center program has developed an array of techniques to improve energy efficiency in industrial facilities. This chapter discusses recommended assessment procedures and observed energy-saving opportunities for some of the most common industrial energy systems. These systems include lighting, compressed air, boilers and steam systems, manufacturing process heating, HVAC, pumps, and fans. Implementation of these assessment recommendations has been demonstrated to increase efficiency and to thus reduce energy consumption and associated costs. While every manufacturing facility is different, and their component industrial energy systems equally unique, this chapter presents a set of analytical guidelines that can be used as a template by engineering practitioners to evaluate their facility energy use and implement subsequent energy conservation measures.",book:{id:"5361",slug:"energy-efficient-buildings",title:"Energy Efficient Buildings",fullTitle:"Energy Efficient Buildings"},signatures:"Gary P. Moynihan and Frank L. 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However, given the high thermal conductivity of steel and the lightness of this type of construction, it may also have some drawbacks if not well designed and executed. Therefore, special attention should be given to the LSF building envelope in order to minimize thermal bridges. Moreover, given the usual reduced thermal mass, several strategies could be implemented to increase thermal inertia, consequently reduce indoor temperature fluctuations, enhance the occupants comfort and increase energy efficiency. In this chapter an overview of the main features related to the thermal behaviour and energy efficiency of LSF buildings is provided alongside some related case studies.",book:{id:"5361",slug:"energy-efficient-buildings",title:"Energy Efficient Buildings",fullTitle:"Energy Efficient Buildings"},signatures:"Paulo Santos",authors:[{id:"186441",title:"Prof.",name:"Paulo",middleName:null,surname:"Santos",slug:"paulo-santos",fullName:"Paulo Santos"},{id:"372973",title:"Dr.",name:"Paulo",middleName:null,surname:"Santos",slug:"paulo-santos",fullName:"Paulo Santos"}]},{id:"69674",doi:"10.5772/intechopen.89821",title:"Wind Turbine Airfoil Boundary Layer Optimization Using Genetic Algorithm with 3D Rotational Augmentation",slug:"wind-turbine-airfoil-boundary-layer-optimization-using-genetic-algorithm-with-3d-rotational-augmenta",totalDownloads:538,totalCrossrefCites:1,totalDimensionsCites:3,abstract:"The airfoil shape of horizontal axis wind turbine (HAWT) blade is optimized using genetic algorithm (GA). The algorithm is set to find the final airfoil shape with the highest gliding ratio (GR) and larger laminar boundary layer regime along the airfoil surface. The main aim is to find the best airfoil shape of higher lift coefficient with reduced drag in boundary layer from the reference airfoil shape. A 3D correction law is applied to model the effect of optimized airfoil in 3D rotational augmented situation. The thrust and power curves are generated by the blade element (BEM) and free vortex (FV) codes with 3D and loss correction. The higher power production is given when the wind turbine blades are designed using the optimized airfoil. This increment is thought to be made from the efficiency caused by the reduced separation bubbles from reduced turbulent boundary layer and 3D rotational augmentation. To validate its effectiveness in case of soiled condition, the aerodynamic parameters of airfoils are recalculated by enforcing the airfoil to undergo earlier transition, which models the leading edge roughness. The results indicate the soiled condition that does not affect the aerodynamic efficiency of the airfoil due to the positive effect of 3D rotation augmentation.",book:{id:"8890",slug:"design-optimization-of-wind-energy-conversion-systems-with-applications",title:"Design Optimization of Wind Energy Conversion Systems with Applications",fullTitle:"Design Optimization of Wind Energy Conversion Systems with Applications"},signatures:"Youjin Kim, Galih Bangga and Antonio Delgado",authors:[{id:"208318",title:"M.Sc.",name:"Youjin",middleName:null,surname:"Kim",slug:"youjin-kim",fullName:"Youjin Kim"},{id:"208321",title:"Prof.",name:"Antonio",middleName:null,surname:"Delgado",slug:"antonio-delgado",fullName:"Antonio Delgado"},{id:"312157",title:"Dr.",name:"Galih",middleName:null,surname:"Bangga",slug:"galih-bangga",fullName:"Galih Bangga"}]},{id:"53729",doi:"10.5772/66669",title:"Building Typology Comparison Between Courtyard and Atrium Buildings: A Study of Thermal Comfort and Energy Performance Factors in Different Climate Zones",slug:"building-typology-comparison-between-courtyard-and-atrium-buildings-a-study-of-thermal-comfort-and-e",totalDownloads:2131,totalCrossrefCites:0,totalDimensionsCites:3,abstract:"The aim of the study in this chapter is to investigate performances shown by courtyard buildings, used widely both as microclimate regulators and as city-wide climate stabilizers especially in the hot-dry climate regions. Furthermore, this study examines atrium buildings having an increasing usage rate in recent years and the presence of comfort problems in particular which have not been resolved for different climate regions. Wind velocity measurements are performed in 36 different points determined in X and Y directions and 17 different points in the Z dimension on the outside of the courtyard considered in this study. In addition, both atrium building typology model and courtyard building typology model are obtained by taking the average courtyard dimensions seen in many regions; by covering open space courtyard section of the geometry with a transparent glass, atrium and courtyard typologies can be obtained. Furthermore, thermal comfort states and energy performances of these two different building typologies in interior courtyard and in building internal volumes for hot-dry, hot-humid and cold climate region conditions as well as the effect of solar radiation values exposing the building surfaces and solar movements during the day on the thermal performance on the building are analysed with CFD FloEFD and Star CCM+ software.",book:{id:"5361",slug:"energy-efficient-buildings",title:"Energy Efficient Buildings",fullTitle:"Energy Efficient Buildings"},signatures:"Enes Yasa",authors:[{id:"185967",title:"Associate Prof.",name:"Enes",middleName:null,surname:"Yasa",slug:"enes-yasa",fullName:"Enes Yasa"},{id:"374708",title:"Dr.",name:"Enes",middleName:null,surname:"Yasa",slug:"enes-yasa",fullName:"Enes Yasa"}]}],mostDownloadedChaptersLast30Days:[{id:"53557",title:"Energy-Efficient Building Design in the Context of Building Life Cycle",slug:"energy-efficient-building-design-in-the-context-of-building-life-cycle",totalDownloads:5469,totalCrossrefCites:19,totalDimensionsCites:29,abstract:"Energy is one of the most important catalysts in wealth generation, economic growth, and social development in all countries. Buildings have a significant share in total energy consumed globally; therefore, they have a profound impact upon the environment. Energy is used in every stage of building life cycle (these stages are choice of locality, architectural design, structural systems and material selection, building construction, usage and maintenance, demolition, reuse-regain-recycle, and waste disposal). According to World Watch Institute data, buildings are responsible for the annual consumption of 40% of the world's energy. Energy consumption of buildings can be reduced significantly in every stage of a building life cycle. This study investigated the energy-efficient methods in building life cycle. In this context, we give information about the life cycle of building and explain energy-efficient guiding principles in life cycle stages.",book:{id:"5361",slug:"energy-efficient-buildings",title:"Energy Efficient Buildings",fullTitle:"Energy Efficient Buildings"},signatures:"Izzet Yüksek and Tülay Tikansak Karadayi",authors:[{id:"186397",title:"Dr.",name:"İzzet",middleName:null,surname:"Yüksek",slug:"izzet-yuksek",fullName:"İzzet Yüksek"},{id:"186398",title:"Prof.",name:"Tülay",middleName:null,surname:"Tıkansak Karadayı",slug:"tulay-tikansak-karadayi",fullName:"Tülay Tıkansak Karadayı"},{id:"374197",title:"Dr.",name:"Izzet",middleName:null,surname:"Yüksek",slug:"izzet-yuksek",fullName:"Izzet Yüksek"},{id:"374198",title:"Dr.",name:"Tülay Tikansak",middleName:null,surname:"Karadayi",slug:"tulay-tikansak-karadayi",fullName:"Tülay Tikansak Karadayi"}]},{id:"53060",title:"Energy Efficiency of Lightweight Steel-Framed Buildings",slug:"energy-efficiency-of-lightweight-steel-framed-buildings",totalDownloads:2788,totalCrossrefCites:1,totalDimensionsCites:6,abstract:"The market share of lightweight steel‐framed (LSF) construction system has grown over the last decades, mainly in low‐rise residential buildings, due to its advantages such as having small weight with high mechanical strength; reduced disruption on‐site and speed of construction; great potential for recycling and reuse; high architectural flexibility for retrofitting purposes; easy prefabrication, allowing modular construction; economy in transportation and handling; superior quality given off‐site manufacture control; and excellent stability of shape in case of humidity and resistance to insect damage. However, given the high thermal conductivity of steel and the lightness of this type of construction, it may also have some drawbacks if not well designed and executed. Therefore, special attention should be given to the LSF building envelope in order to minimize thermal bridges. Moreover, given the usual reduced thermal mass, several strategies could be implemented to increase thermal inertia, consequently reduce indoor temperature fluctuations, enhance the occupants comfort and increase energy efficiency. In this chapter an overview of the main features related to the thermal behaviour and energy efficiency of LSF buildings is provided alongside some related case studies.",book:{id:"5361",slug:"energy-efficient-buildings",title:"Energy Efficient Buildings",fullTitle:"Energy Efficient Buildings"},signatures:"Paulo Santos",authors:[{id:"186441",title:"Prof.",name:"Paulo",middleName:null,surname:"Santos",slug:"paulo-santos",fullName:"Paulo Santos"},{id:"372973",title:"Dr.",name:"Paulo",middleName:null,surname:"Santos",slug:"paulo-santos",fullName:"Paulo Santos"}]},{id:"51988",title:"Energy Efficiency in Manufacturing Facilities: Assessment, Analysis and Implementation",slug:"energy-efficiency-in-manufacturing-facilities-assessment-analysis-and-implementation",totalDownloads:2532,totalCrossrefCites:5,totalDimensionsCites:7,abstract:"Manufacturing facilities are one among the largest consumers of energy. Efforts to improve energy efficiency are an increasing concern for many manufacturing facility engineering managers. This can be achieved by evaluating energy end uses (e.g., lighting, processing equipment, and heating, air conditioning, and ventilation (HVAC) systems), and by implementing measures to reduce the total amount of energy consumed for one or more of the end uses. Throughout the 40 years of its existence, the US Department of Energy’s Industrial Assessment Center program has developed an array of techniques to improve energy efficiency in industrial facilities. This chapter discusses recommended assessment procedures and observed energy-saving opportunities for some of the most common industrial energy systems. These systems include lighting, compressed air, boilers and steam systems, manufacturing process heating, HVAC, pumps, and fans. Implementation of these assessment recommendations has been demonstrated to increase efficiency and to thus reduce energy consumption and associated costs. While every manufacturing facility is different, and their component industrial energy systems equally unique, this chapter presents a set of analytical guidelines that can be used as a template by engineering practitioners to evaluate their facility energy use and implement subsequent energy conservation measures.",book:{id:"5361",slug:"energy-efficient-buildings",title:"Energy Efficient Buildings",fullTitle:"Energy Efficient Buildings"},signatures:"Gary P. Moynihan and Frank L. Barringer",authors:[{id:"16974",title:"Dr.",name:"Gary",middleName:null,surname:"Moynihan",slug:"gary-moynihan",fullName:"Gary Moynihan"},{id:"193958",title:"Mr.",name:"Frank",middleName:null,surname:"Barringer",slug:"frank-barringer",fullName:"Frank Barringer"},{id:"371713",title:"Dr.",name:"Frank L.",middleName:null,surname:"Barringer",slug:"frank-l.-barringer",fullName:"Frank L. Barringer"}]},{id:"53729",title:"Building Typology Comparison Between Courtyard and Atrium Buildings: A Study of Thermal Comfort and Energy Performance Factors in Different Climate Zones",slug:"building-typology-comparison-between-courtyard-and-atrium-buildings-a-study-of-thermal-comfort-and-e",totalDownloads:2129,totalCrossrefCites:0,totalDimensionsCites:3,abstract:"The aim of the study in this chapter is to investigate performances shown by courtyard buildings, used widely both as microclimate regulators and as city-wide climate stabilizers especially in the hot-dry climate regions. Furthermore, this study examines atrium buildings having an increasing usage rate in recent years and the presence of comfort problems in particular which have not been resolved for different climate regions. Wind velocity measurements are performed in 36 different points determined in X and Y directions and 17 different points in the Z dimension on the outside of the courtyard considered in this study. In addition, both atrium building typology model and courtyard building typology model are obtained by taking the average courtyard dimensions seen in many regions; by covering open space courtyard section of the geometry with a transparent glass, atrium and courtyard typologies can be obtained. Furthermore, thermal comfort states and energy performances of these two different building typologies in interior courtyard and in building internal volumes for hot-dry, hot-humid and cold climate region conditions as well as the effect of solar radiation values exposing the building surfaces and solar movements during the day on the thermal performance on the building are analysed with CFD FloEFD and Star CCM+ software.",book:{id:"5361",slug:"energy-efficient-buildings",title:"Energy Efficient Buildings",fullTitle:"Energy Efficient Buildings"},signatures:"Enes Yasa",authors:[{id:"185967",title:"Associate Prof.",name:"Enes",middleName:null,surname:"Yasa",slug:"enes-yasa",fullName:"Enes Yasa"},{id:"374708",title:"Dr.",name:"Enes",middleName:null,surname:"Yasa",slug:"enes-yasa",fullName:"Enes Yasa"}]},{id:"71507",title:"Structural Optimization of Wind Turbine Blades for Improved Dynamic Performance",slug:"structural-optimization-of-wind-turbine-blades-for-improved-dynamic-performance",totalDownloads:837,totalCrossrefCites:0,totalDimensionsCites:0,abstract:"The design of the main structure of a wind turbine blade is optimized aiming at the improvement of the overall dynamic performance. Three optimization strategies are developed and tested. The first fundamental one is based on minimizing the total structural mass of the blade spar under frequency and strength constraints. The second and third strategies are concerned with the reduction of the overall vibration level by either minimizing a frequency-placement index or maximizing the natural frequencies and placing them at their target values to avoid large amplitudes and resonance occurrence. Design variables include cross-sectional dimensions and material properties along the spanwise direction of the blade spar. The optimization problem is formulated as a nonlinear constrained problem solved by sequential quadratic programming (SQP) technique. Two specific layup configurations, namely, circumferentially asymmetric stiffness (\nCAS\n) and circumferentially uniform stiffness (\nCUS\n), are analyzed. Exact analytical methods are applied to calculate the natural modes of vibration of a composite, thin-walled, tapered blade spar. The influence of coupling on the vibration modes is identified, and the functional behavior of the frequencies with the lamination parameters is thoroughly investigated and discussed. Finite element modeling using NX Nastran solver is performed in order to validate the analytical results. As a case study, optimized blade spar designs of a 750-kW horizontal axis wind turbine are given. The attained solutions show that the approach used in this study enhances the dynamic characteristics of the optimized spar structures as compared with a known baseline design of the wind turbine blade.",book:{id:"8890",slug:"design-optimization-of-wind-energy-conversion-systems-with-applications",title:"Design Optimization of Wind Energy Conversion Systems with Applications",fullTitle:"Design Optimization of Wind Energy Conversion Systems with Applications"},signatures:"Gerges Edwar Mehanny Beshay and Karam Yousef Maalawi",authors:[{id:"150041",title:"Prof.",name:"Karam",middleName:"Youssef",surname:"Maalawi",slug:"karam-maalawi",fullName:"Karam Maalawi"},{id:"282747",title:"Dr.",name:"Gerges",middleName:"Edwar",surname:"Beshay",slug:"gerges-beshay",fullName:"Gerges Beshay"}]}],onlineFirstChaptersFilter:{topicId:"764",limit:6,offset:0},onlineFirstChaptersCollection:[],onlineFirstChaptersTotal:0},preDownload:{success:null,errors:{}},subscriptionForm:{success:null,errors:{}},aboutIntechopen:{},privacyPolicy:{},peerReviewing:{},howOpenAccessPublishingWithIntechopenWorks:{},sponsorshipBooks:{sponsorshipBooks:[],offset:8,limit:8,total:0},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:104,numberOfOpenTopics:3,numberOfUpcomingTopics:0,issn:"2631-5343",doi:"10.5772/intechopen.71985",isOpenForSubmission:!0}],lsSeriesList:[{id:"11",title:"Biochemistry",numberOfPublishedBooks:32,numberOfPublishedChapters:320,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2632-0983",doi:"10.5772/intechopen.72877",isOpenForSubmission:!0},{id:"25",title:"Environmental Sciences",numberOfPublishedBooks:1,numberOfPublishedChapters:12,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2754-6713",doi:"10.5772/intechopen.100362",isOpenForSubmission:!0},{id:"10",title:"Physiology",numberOfPublishedBooks:11,numberOfPublishedChapters:141,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2631-8261",doi:"10.5772/intechopen.72796",isOpenForSubmission:!0}],hsSeriesList:[{id:"3",title:"Dentistry",numberOfPublishedBooks:8,numberOfPublishedChapters:133,numberOfOpenTopics:2,numberOfUpcomingTopics:0,issn:"2631-6218",doi:"10.5772/intechopen.71199",isOpenForSubmission:!0},{id:"6",title:"Infectious Diseases",numberOfPublishedBooks:13,numberOfPublishedChapters:113,numberOfOpenTopics:3,numberOfUpcomingTopics:1,issn:"2631-6188",doi:"10.5772/intechopen.71852",isOpenForSubmission:!0},{id:"13",title:"Veterinary Medicine and Science",numberOfPublishedBooks:11,numberOfPublishedChapters:107,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:19,numberOfOpenTopics:3,numberOfUpcomingTopics:0,issn:"2753-894X",doi:"10.5772/intechopen.100359",isOpenForSubmission:!0},{id:"23",title:"Education and Human Development",numberOfPublishedBooks:0,numberOfPublishedChapters:5,numberOfOpenTopics:1,numberOfUpcomingTopics:1,issn:null,doi:"10.5772/intechopen.100360",isOpenForSubmission:!0},{id:"24",title:"Sustainable Development",numberOfPublishedBooks:0,numberOfPublishedChapters:16,numberOfOpenTopics:5,numberOfUpcomingTopics:0,issn:null,doi:"10.5772/intechopen.100361",isOpenForSubmission:!0}],testimonialsList:[{id:"13",text:"The collaboration with and support of the technical staff of IntechOpen is fantastic. The whole process of submitting an article and editing of the submitted article goes extremely smooth and fast, the number of reads and downloads of chapters is high, and the contributions are also frequently cited.",author:{id:"55578",name:"Antonio",surname:"Jurado-Navas",institutionString:null,profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bRisIQAS/Profile_Picture_1626166543950",slug:"antonio-jurado-navas",institution:{id:"720",name:"University of Malaga",country:{id:null,name:"Spain"}}}},{id:"6",text:"It is great to work with the IntechOpen to produce a worthwhile collection of research that also becomes a great educational resource and guide for future research endeavors.",author:{id:"259298",name:"Edward",surname:"Narayan",institutionString:null,profilePictureURL:"https://mts.intechopen.com/storage/users/259298/images/system/259298.jpeg",slug:"edward-narayan",institution:{id:"3",name:"University of Queensland",country:{id:null,name:"Australia"}}}}]},series:{item:{id:"25",title:"Environmental Sciences",doi:"10.5772/intechopen.100362",issn:"2754-6713",scope:"\r\n\tScientists have long researched to understand the environment and man’s place in it. 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We encourage the submission of manuscripts that provide novel and mechanistic insights that report significant advances in the fields. Topics include, but are not limited to: Advanced techniques of cellular and molecular biology (Molecular methodologies, imaging techniques, and bioinformatics); Biological activities at the molecular level; Biological processes of cell functions, cell division, senescence, maintenance, and cell death; Biomolecules interactions; Cancer; Cell biology; Chemical biology; Computational biology; Cytochemistry; Developmental biology; Disease mechanisms and therapeutics; DNA, and RNA metabolism; Gene functions, genetics, and genomics; Genetics; Immunology; Medical microbiology; Molecular biology; Molecular genetics; Molecular processes of cell and organelle dynamics; Neuroscience; Protein biosynthesis, degradation, and functions; Regulation of molecular interactions in a cell; Signalling networks and system biology; Structural biology; Virology and microbiology.",coverUrl:"https://cdn.intechopen.com/series_topics/covers/14.jpg",keywords:"Omics (Transcriptomics; Proteomics; Metabolomics), Molecular Biology, Cell Biology, Signal Transduction and Regulation, Cell Growth and Differentiation, Apoptosis, Necroptosis, Ferroptosis, Autophagy, Cell Cycle, Macromolecules and Complexes, Gene Expression"},{id:"15",title:"Chemical Biology",scope:"Chemical biology spans the fields of chemistry and biology involving the application of biological and chemical molecules and techniques. 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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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Dr. Blumenberg’s research is focused on the epidermis, expression of keratin genes, transcription profiling, keratinocyte differentiation, inflammatory diseases and cancers, and most recently the effects of the microbiome on the skin. 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Topics include, but are not limited to: Advanced techniques of cellular and molecular biology (Molecular methodologies, imaging techniques, and bioinformatics); Biological activities at the molecular level; Biological processes of cell functions, cell division, senescence, maintenance, and cell death; Biomolecules interactions; Cancer; Cell biology; Chemical biology; Computational biology; Cytochemistry; Developmental biology; Disease mechanisms and therapeutics; DNA, and RNA metabolism; Gene functions, genetics, and genomics; Genetics; Immunology; Medical microbiology; Molecular biology; Molecular genetics; Molecular processes of cell and organelle dynamics; Neuroscience; Protein biosynthesis, degradation, and functions; Regulation of molecular interactions in a cell; Signalling networks and system biology; Structural biology; Virology and microbiology.",annualVolume:11410,isOpenForSubmission:!0,coverUrl:"https://cdn.intechopen.com/series_topics/covers/14.jpg",editor:{id:"165627",title:"Dr.",name:"Rosa María",middleName:null,surname:"Martínez-Espinosa",fullName:"Rosa María Martínez-Espinosa",profilePictureURL:"https://mts.intechopen.com/storage/users/165627/images/system/165627.jpeg",institutionString:null,institution:{name:"University of Alicante",institutionURL:null,country:{name:"Spain"}}},editorTwo:null,editorThree:null,editorialBoard:[{id:"79367",title:"Dr.",name:"Ana Isabel",middleName:null,surname:"Flores",fullName:"Ana Isabel Flores",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bRpIOQA0/Profile_Picture_1632418099564",institutionString:null,institution:{name:"Hospital Universitario 12 De Octubre",institutionURL:null,country:{name:"Spain"}}},{id:"328234",title:"Ph.D.",name:"Christian",middleName:null,surname:"Palavecino",fullName:"Christian Palavecino",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0033Y000030DhEhQAK/Profile_Picture_1628835318625",institutionString:null,institution:{name:"Central University of Chile",institutionURL:null,country:{name:"Chile"}}},{id:"186585",title:"Dr.",name:"Francisco Javier",middleName:null,surname:"Martin-Romero",fullName:"Francisco Javier Martin-Romero",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bSB3HQAW/Profile_Picture_1631258137641",institutionString:null,institution:{name:"University of Extremadura",institutionURL:null,country:{name:"Spain"}}}]},{id:"15",title:"Chemical Biology",keywords:"Phenolic Compounds, Essential Oils, Modification of Biomolecules, Glycobiology, Combinatorial Chemistry, Therapeutic peptides, Enzyme Inhibitors",scope:"Chemical biology spans the fields of chemistry and biology involving the application of biological and chemical molecules and techniques. 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Behind these definitions are hidden all the aspects of normal and pathological functioning of all processes that the topic ‘Metabolism’ will cover within the Biochemistry Series. 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Thus proteomics, an area of research that detects all protein forms expressed in an organism, including splice isoforms and post-translational modifications, is more suitable than genomics for a comprehensive understanding of the biochemical processes that govern life. The most common proteomics applications are currently in the clinical field for the identification, in a variety of biological matrices, of biomarkers for diagnosis and therapeutic intervention of disorders. From the comparison of proteomic profiles of control and disease or different physiological states, which may emerge, changes in protein expression can provide new insights into the roles played by some proteins in human pathologies. Understanding how proteins function and interact with each other is another goal of proteomics that makes this approach even more intriguing. Specialized technology and expertise are required to assess the proteome of any biological sample. 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