Elastic, Optical, Transport, and Structural Properties of GaAs

Open access peer-reviewed chapter

Submitted: 17 August 2020 Reviewed: 20 October 2020 Published: 06 November 2020

DOI: 10.5772/intechopen.94566

One of the major objectives of physics is to understand the physical properties of compound metals. Based on this very objective, in this chapter, we intend to review the physical as well as chemical properties of Gallium Arsenide material.

• GaAs
• basic principle
• physical properties
• optical properties
• chemical properties
• physics

Each time the creation and refinement of new material growth techniques give rise to the finding of new equipment. The semiconductor which has been found to be most interesting of all (when used), relates to the applications in electronic devices for instance, high speed circuits formed of group III-V compounds along with switches or amplifiers. One of the types of is the Gallium Arsenide (GaAs) [1, 2]. A III-V semiconductor that it is, its composition includes gallium which is an element of the group 3 having orthorhombic trigonal crystal structure coupled with arsenic which belongs to the group 5 and has a trigonal crystal structure. This very combination leads to interesting physical as well as chemical properties in this semiconductor [3, 4]. With different electronic band gaps, these semiconductors can, at ambient temperatures, crystalize into a zinc-blende cubic type crystal structure. Post the discovery of transistor in the year 1947, Gallium arsenide (GaAs) has presented itself as a prominent material for electronic devices. The technological importance and the need of study of Gallium arsenide (GaAs) in the last few years are due to its high melting point at 1238° C along with a density of 5.3176 g/cm3. It is obtained as a by-product from the extraction of ores of zinc and aluminum and is present at 5-15 mg/Kg in Earth’s crust [5, 6].

GaAs is the basis of a worldwide industry it has a wide usage area changing from microwave frequency integrated circuits to optical windows. Among III-V semiconductors, GaAs has remained useful as a semiconductor material, widely being used in optoelectronic and microelectronic devices. Given this wide use of GaAs, the idea came to write this chapter focusing on the physical and chemical properties of this important material. While excluding the impurities present and their associated effects, the focus is on the characteristics of GaAs [7, 8].

Included in this chapter, are a few physical as well as chemical properties of gallium arsenide (GaAs) such as the crystal Structure, the direct bandgap of GaAs with its zinc blende type crystal structure, electronic structure, light-emitting properties, electromagnetic properties, photovoltaic properties, phase transition and mechanical as well as elastic properties. The geometric structures, stabilities, and electronic properties like higher saturated electron velocity and high carrier mobility with a small dielectric constant and high resistivity. This chapter also elaborates on the thermodynamic properties of GaAs such as thermal expansion and thermal conduction.

These great properties led to the production of new and unique devices like high-efficiency light emitters, light sensors, and high-speed switching devices. The GaAs is considered as an outstanding member of the III-V semiconductor family. It has many exceptional features, especially for the recent optoelectronic industry. Hence, special focus has been laid on the examination of physical properties of this material [9, 10, 11].

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The band structure is the major part of the semiconductors. Briefly explaining it, at absolute zero, a bandgap or an energy gap separates the conduction band (lowest empty band) with the valence band (highest filled band). Therefore, at T = 0, electricity is not conducted by the material. The electrons are enabled to be excited into the conduction band through several processes, such as optical absorption or thermal excitation, at finite temperatures and electrical conduction is allowed as there are empty states in the valence band. Energy, in the forms of heat or photons, is released when the electrons return to the valence band [12, 13].

As mentioned in Figure 1, two types of bandgaps are there based on different conditions. The first one is if, over the top of the valence bond, the bottom of the conduction band does not rest. As a result of this, it is called an indirect gap. Also, photon is necessary in order to provide the momentum required to reach the state in the conduction band, and the electronic transition to happen. However, in case of GaAs and other direct band type semiconductor, the bottom of the conduction band site and the top of the valence band are on top of each other, Therefore even without a change in the wave vector, the electron is able to get excited from the valence band. A photon on absorbing required energy is sufficient enough for this. Moreover, through the emission of a photon, transition to the valence band from the conduction band can easily be done by the electron. While no interaction of photon is required, emission of light energy of the desired wavelength of 850 nm bandgap occurs and it allows the direct band recombination of holes and electrons. In the absence of defects, the energy released by the dominant mechanism of the indirect bandgap is by photons via electromagnetic radiation. However, photons release energy in the form of heat in the case of indirect bandgap semiconductors [14, 15, 16].

Schematic of the valence band, direct bandgap, and indirect bandgap conduction bands [13].

Being a good optoelectronic material, direct bandgap in GaAs is considered a useful material in the field of optoelectronics and other electronic fields and is used comprehensively in semiconductor lasers as well as light-emitting diodes. Its use has also been encouraged in the making of high-efficiency solar cells, Gunn diodes, Infrared LEDs, solid-state detectors and radar systems. We have a classification of 1–3 categories depending upon the magnitude of bandgap energy of the materials, namely, narrow, mid and wide-bandgap. Of all the properties of a semiconductor, the presence of energy gap leads all others [16, 17].

Not only band-gap engineering permits the making of band diagrams that have continuous as well as arbitrary band-gap variations, but it is also considered among the strongest tools for the new semiconductor devices and materials. For a specific application, the transport properties of holes, as well as electrons, may be continuous and independent. This approach leads us to a new generation of devices having unique capabilities ranging from resonant tunneling transistors to solid-state photomultipliers. More than for any semiconductor, many band structures for GaAs are precisely known. Figures 2 and 3 make it clear, showing 1.519 eV as the fundamental energy gap for Gallium Arsenide. Also, the high-temperature performance of GaAs is largely attributed to its wide bandgap [20, 21, 22].

Structure of GaAs energy band gap [18].

(a) Calculated band structure of GaAs using the tight binding method. (b) Sketch of GaAs band structure near the Γ-symmetry point showing conduction band, heavy hole band (hh), light hole band (lh), and split-off band (so) in the X [100] and L [19].

Other than this, photoconductivity, a feature semiconductor exhibit under suitable trial conditions is another benefit associated with the bandgap [23]. This occurs when an increase in electrical conductivity happens when an incident light falls on a semiconductor. The suitability of the semiconductor material in optoelectronic devices is also decided by its photoconductive response. Such materials which respond well to the photoconductivity, find themselves useful in the making of infrared sold state detectors. Also, in GaAs, the transport properties of hot electrons are largely affected due to the bandgap. Alloying is another controllable bandgap which useful property of the GaAs [22, 24, 25, 26].

The usefulness of GaAs and its alloys in optoelectronics such as sold state lasers and LEDs lies in the bandgap of GaAs which, in the infra-red range results in the emission of photon. The ability of GaAs to retain their semiconductor properties at high temperatures, giving stability to the GaAs comes from the wider bandgap of GaAs [19]. Figure 3 shows that Calculated band structure of GaAs using the tight binding method with different semiconductor materials.

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That GaAs is an extremely poor conductor is corroborated by the fact that GaAs has low flow intrinsic carrier density when present in an undoped or pure form. Hence it is mostly considered as semi-insulating. Adding the dopants of either the p- or the n- that is the positive and the negative types respectively, alters this property. Many active devices have been able to be made on a single substrate due to this semi-insulating property, where each device’s electrical isolation is provided by the GaAs. For contraction of the electronic circuitry, this characteristic has been found be quite important [27, 28].

With regards to the transport properties, two important questions that come up where the incorporation of dopants has been done – a) mobility, b) effective carrier concentration [29, 30].

Nc and NV, the effective density of states at the band edges, are dependent on temperature and the effective mass of the electron and holes respectively.

The conductivity is given by

Eq. (1) and Figure 4 can be used to understand the effect of temperature on the concentration of the carrier. It shows the entry of temperature in both exponential as well as pre-exponential terms. There are two effects of increased temperature [31, 32]:

• the effective density of states of the edge of the band is increased (NV and NC).

• the exponential portion of Eq. 10 shows a decrease, since its denominator is T.

Bandgap energy inverse T for Ge, Si, GaAs in the range 200–1000 K. T [31].

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In solid-state physics, the central theoretical problem happens to be the determination of the energy bands. In other words, in case of solids, the central theoretical problem is the calculation of energy levels of electrons. In order to calculate physical properties such as mechanical properties, magnetic order, optical dielectric or the vibrational spectra, in principle knowledge of the electrons and the energies associated with them is required. In contrast, calculation of lattice constants and other bulk ground state properties such as atomic positions and bulk modulus is considered to be important in physics associated with condensed matter. Such bulk calculations not only help understand as well as characterize the mechanical properties of the matter, but they also help predict their properties in extreme conditions [33, 34, 35].

Having a basis and a cubic lattice that is two face centered, the structure of crystal of GaAs is a zincblende structure or cubic sphalerite. In the classic basis, at the origin of the lattice, there is one GaAs molecule. From (0,0,0), the vector of one atom to another at (1/4,1/4,1/4) of the molecule constitutes the basis. Two FCC lattices, one of as while the other being of Ga can also form a crystal as shown in Figure 5. While arsenic atoms are represented in orange color, the Gallium ones are shown in purple color. As shown, there are 4 arsenic atoms against 14 gallium atoms. This makes a tetrahedral bond, similar to the one in a diamond lattice, but replaced with Ga and as where each Ga is connected to four other atoms. It shows ionic bonding with the presence of two types of atoms [37, 38, 39] (Figure 6).

P-V plot of GaAs up to 25 GPA [36].

The crystal structure of GaAs cubic unit cell of GaAs [38].

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Figure 7 shows that the drawing of the energy band of the semiconductor, which demonstrates the bandgap along with valence and conduction electrons. An electron leaves a hole in the valence band on moving to the conduction band from the valence band. For the other electrons in the valence band energy levels, this hole is an empty state and behaves in a manner similar to a +ve charged particle in the valence band. The number of electrons in the conduction band per unit volume, written as cm3, is counted to quantify the electron concentration, and is represented by ‘n’ [41, 42].

Room-temperature band gap energy, Eg, as a function of lattice constant for several semiconductors. Lines connecting binary compounds such as GaAs and AlAs represent alloy composition with either a direct band gap (thick solid line) or indirect band gap (thin red line). The III–V and II–VI semiconductor compounds in the figure have the zinc blende crystal structure. Si and Ge have the diamond crystal structure [40].

The density of holes in the valence band equals the density of electrons in the conduction band.

NC=expEF−ECKBT=NvexpEv−EFKbTE5

In the above formula,

EF - Fermi energy.

NV - effective density of states in the valence band.

EV - valence band edge.

kB - Boltzmann’s constant.

EC - conduction band edge.

T - temperature in K.

NC - effective density of states in the conduction band.

Reordering the above equation, we have

Taking log we have

Solving for EF

It is in the middle of the bandgap that we have the Fermi energy (EC + EV)/2. Therefore, as shown in 7, the energy bandgap latticed matched for several semiconductors that is related to GaAs and band alignments for sever III-V semiconductor with GaAs (Figure 8).

Band alignments for sever III-V semiconductor with GaAs. (a) Lattice constants and band gaps of different semiconductor materials. The lattice constants of Ge and GaAs are close to a variety of semiconductors with different band gaps, thereby commonly used as substrates for tandem cells. (b) Schematics of a triple-junction tandem cell with optimized compositions of InGaAs and InGaP, which correspond to the blue dots in (a). A buffer layer has to be applied to accommodate the lattice mismatch between the Ge substrate and In 0.17 Ga 0.83 As; (c) Proposed latticematched GeSn/InGaAs/InGaP tandem cell [42].

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An ionic bond exists between the electrons in the valence band of GaAs atoms. Therefore, in solids, they are not free to transport. However, they can move through a solid if the electron gets excited to the conduction band. Hence, an electron leaves a hole in the valence band on moving to the conduction band from the valence band. An electron jump from one bond to another enables the hole to move in the valence band. Further, these holes and electrons can move upon affected by an electric field [43, 44, 45].

The equation that helps derive the acceleration of the electrons (ae) is-

Where me is the electron’s rest mass and EX is the electric field. Under an electric field, the interaction of electrons with the solid atoms should also be considered.

In the case of an electron in a solid, under an external field, the interaction with the solid atoms should also be taken into account. Let this interaction of electrons with the atoms of the solid be summed up as ∑fint [46, 47].

The conduction electrons are initially in the lowest energy valley, Γ minimum. Here, they are distinguished by a low effective mass and have high mobility. On applying the electric field, these electrons are rapidly accelerated by the field to high velocities: they gain kinetic energy. The electrons’ ability gains enough energy to transfer from this valley to the next higher valley, the L minimum. These upper valleys are distinguished by a larger effective mass, and consequently both lower electron mobility and a greater density of available electron positions. The great density of states encourages transfer to these valleys of electrons with suitable energy. There is a fall in the average velocity of all the electrons as the energetic electrons transfer to the upper levels. There is much work available which is focused on the calculation of hot electron transport properties in GaAs. Gallium arsenide exhibits the `transferred electron’ which is commonly known as the TE effect. This transfer of electrons from one region to another energy band structure is an electric-induced field transfer. It has high electron mobility, with a negative resistance being observed and has a small dielectric constant. This is primarily because of extensive utilization of GaAs in ultrahigh frequency, high-temperature resistance and low power circuits and devices [48, 49, 50, 51, 52, 53].

average velocityν=nΓνΓ+nrνrnΓ+nlE11

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There are two main categories in which the optoelectronic devices can be categorized. First is the set of those devices in which electrical current get converted into electromagnetic radiation i.e. light. Second is the set of those devices in which light is converted into electric current. An example of the first category of devices is the LEDs. Optoelectronic devices as well as light-emitting devices have GaAs in them. Macroscopic evidence is available for the interaction of matter with light and it is made of four components, namely, incident, reflected, transmitted, and scattered component [52, 54, 55].

Absorption of a photon in a semiconductor can happen in a number of ways. This is commonly known as interbond absorption. This happens when in the conduction band an electron is excited up after having absorbed a photon in the valence band. The momentum is unchanged in case of direct gap semiconductor while there is an increase in electron’s energy. The momentum is though shifted in case of an indirect gap material. This is made possible by a decrease in bandgap energy with the increase in temperature and a photon being either absorbed or emitted. The two factors responsible for this are lattice vibration (phonons) and thermal expansion. The increase of lattice constant is due to the thermal expansion. This further leads to the change in the periodic potential as seen by the electron. The band structure is altered due to these changes [56, 57, 58, 59].

Temperature and bandgap shift are related as per the following formula

where

Eg - band gap energy

T - temperature

Eg (0) - bandgap at 0 K having units same as that of energy

α has units the same as that of temperature/energy.

Prominently used in optoelectronic as well as microelectronic devices, Gallium arsenide, GaAs is considered a good semiconducting material, having high electron mobility. In the semiconductor material, through the interaction of electron and photons, sunlight is converted into electricity directly by photovoltaic cells [60, 61, 62].

Electronic excitation of luminescence is the reason, it is also called as optical radiation. State energy is emitted in the form of EM radiation when the excited electrons move back to the ground. Depending upon the electronic excitation created originally, there are four different types of luminescence, namely,

Photoluminescence−incident light→electronic excitation

Radioluminescence−ionizing radiationβ−rays→electronic excitation

Cathodoluminescence−electron beam→electronic excitation

Electroluminescence−electrical field→electronic excitation

The functioning of LEDs is by electroluminescence. Using a functional bias, electric current which includes holes and electrons are forwarded to the device. Light is emitted by the recombination of these holes and electrons. In order to increase efficiency, heterostructure LEDs are used. The holes and the electrons, collectively called the carriers are confined in a small spatial region in order to achieve this. Due to the localization of carriers in GaAs, there is higher quantum efficiency at the heterojunction. Hence, it is only in the i-GaAs region, that the recombination takes place. Figure 9 draws a clear picture of the emitted wavelength in case of both LEDs as shown in Figure 9 [63, 64, 65, 66].

The heterojunction has a higher quantum efficiency since the carriers are localized GaAs [63].

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The physical knowledge of the materials namely the phase transitions, interatomic forces and the mechanical features apart from many other features are better understood by examining the elastic properties of the material.

Being low-density materials, III-V compounds, under pressure, have the ability to show transitions of structural phase to a phase with higher density. Figure 3 clearly shows that with increase in pressure, the density of GaAs also increases [67].

Figure 5 shows the P-V graph which helps determine the B3 → B1 phase transition of GaAs. At 17 GPa there is an unexpected decrease in the GaAs’s volume. This decrease is attributed to the change in the structural phase related with phase transition of B3 → B1 [23, 36, 68, 69, 70, 71].

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Gallium Arsenide is deemed as an eminent member of the III-V semiconductor group. It has presented itself as a notable material for electronic devices and vastly being used in optoelectronic and microelectronic devices. The precept knowledge of the electrons and the energies related to GaAs is required in order to calculate physical properties. Furthermore, calculation of lattice constants and other bulk ground state properties is considered to be paramount in physics associated with condensed matter.

In this chapter we have reported the basic principle for the GaAs material as well as the physical, optical, and chemical properties. Also, we have reported the crystal growth of the GaAs with another semiconductor material such as In and Al.

1. 1. Aleshkin VY, Dubinov AA. Direct band Ge and Ge/InGaAs quantum wells in GaAs. J Appl Phys. 2011;109(12):4–9
2. 2. Bickford JR. Doped Aluminum Gallium Arsenide ( AlGaAs )/ Gallium Arsenide ( GaAs ) Photoconductive Semiconductor Switch ( PCSS ) Fabrication. 2016;
3. 3. Scrap A, Cheng T, Liu C, Tsai T, Shen Y. A Process for the Recovery of Gallium from Gallium. 2019;
4. 4. Fang SF, Adomi K, Iyer S, Morkoç H, Zabel H, Choi C, et al. Gallium arsenide and other compound semiconductors on silicon. J Appl Phys. 1990;68(7)
5. 5. Kasap S, Capper. Gallium Arsen. 2006;499–536
6. 6. Kurt HH. The Features of GaAs and GaP Semiconductor Cathodes in an Infrared Converter System. 2018;(May 2017)
7. 7. Kurt HH, Tanrıverdi E. The Features of GaAs and GaP Semiconductor Cathodes in an Infrared Converter System. J Electron Mater. 2017;46(7):4024–33
8. 8. Price GL. Gallium Arsenide and Related Compounds. Met forum. 1984;7(3):171–86
9. 9. Güler E, Güler M. Phase Transition and Elasticity of Gallium Arsenide under Pressure 2 . Computational Details. 2014;17(5):1268–72
10. 10. Nugroho MB. Semoconductor Bandstructure. J Chem Inf Model. 2013;53(9):1689–99
11. 11. Ashby, C., Baca, A. and Institution of Electrical Engineers., 2005. Fabrication Of Gaas Devices (EMIS Processing Series ; No. 6). Institution of Engineering and Technology - IET
12. 12. Electronic Materials, Devices, and Fabrication (Prof. S. Parasuraman, IIT Madras): Lecture 02 - Introduction to Semiconductors
13. 13. Aleshkin, V. Y. and Dubinov, A. A. (2011) ‘Direct band Ge and Ge/InGaAs quantum wells in GaAs’, Journal of Applied Physics, 109(12), pp. 4–9. doi: 10.1063/1.3594753
14. 14. Capasso, F. (1987) ‘Band-Gap Engineering: From Physics and Materials To New Semiconductor Devices.’, Science, 235(4785), pp. 172–176. doi: 10.1126/science.235.4785.172
15. 15. Nayak, C. (2004) ‘Quantum Condensed Matter Physics’, Lecture Notes, pp. 1–17. Available at: http://stationq.cnsi.ucsb.edu/∼nayak/QFT-9-29-2011.pdf
16. 16. WANG, F. F. Y. (1989) ‘Carrier Concentrations’, Introduction to Solid State Electronics, pp. 139–153. doi: 10.1016/b978-0-444-87317-0.50013-7
17. 17. Copple A, Ralston N, Peng X. Engineering direct-indirect band gap transition in wurtzite GaAs nanowires through size and uniaxial strain
18. 18. Nugroho MB. Semoconductor Bandstructure. J Chem Inf Model. 2013;53(9):1689–99
19. 19. Transport E. Density of States, Fermi Energy, and Energy Bands. Thermoelectr Des Mater. 2016;189–205
20. 20. Williamson AJ, Franceschetti A, Fu H, Wang LW, Zunger A. Indirect band gaps in quantum dots made from direct-gap bulk materials. J Electron Mater. 1999;28(5):414–25
21. 21. Electronic Materials, Devices, and Fabrication (Prof. S. Parasuraman, IIT Madras): Lecture 02 - Introduction to Semiconductors
22. 22. Diakite YI, Traore SD, Malozovsky Y, Khamala B, Franklin L, Bagayoko D. Accurate Electronic, Transport, and Bulk Properties of Gallium Arsenide (GaAs)
23. 23. Owolabi JA, Onimisi MY, Abdu SG, Olowomofe GO. Determination of Band Structure of Gallium-Arsenide and Aluminium-Arsenide Using Density Functional Theory. Comput Chem. 2016;04(03):73–82
24. 24. F. Rana Chapter 1 Review of Basic Semiconductor Physics
25. 25. Lou CY, Somorjai GA. Lawrence Berkeley National Laboratory Recent Work Title STUDIES OF THE VAPORIZATION MECHANISM OF GALLIUM ARSENIDE SINGLE CRYSTALS
26. 26. August CL. Carrier Concentrations
27. 27. Fermi energy of an intrinsic semiconductor [Internet]. Available from: https://lampx.tugraz.at/∼hadley/psd/weblectures/Ef_intrinsic/index.php
28. 28. Ashby, C., Baca, A. and Institution of Electrical Engineers., 2005. Fabrication Of Gaas Devices (EMIS Processing Series ; No. 6). Institution of Engineering and Technology - IET
29. 29. Cheng TH, Liu CJ, Tsai TY, Shen YH. A process for the recovery of gallium from gallium arsenide scrap. Processes. 2019;7(12)
30. 30. Güler E, Güler M. Phase Transition and Elasticity of Gallium Arsenide under Pressure. Computational Details. 2014;17(5):1268–72
31. 31. Ghita R V, Negrila CC, Cotirlan C, Logofatu C. ON THE PASSIVATION OF GaAs SURFACE BY SULFIDE COMPOUNDS. Vol. 8, Digest Journal of Nanomaterials and Biostructures
32. 32. Kayali S. I. GaAs Material Properties. Kabita K, Maibam J, Sharma BI, Brojen Singh RK, Thapa RK. Density functional theory study on pressure induced structural transformation, elastic properties and electronic structure of gallium arsenide (GaAs) . Vol. 8, International Journal of Innovation and Applied Studies. 2014
33. 33. Flannery CM, Chilla E, Semenov S, Froehlich HJ. Elastic properties of GaAs obtained by inversion of laser-generated surface acoustic wave measurements. In: Proceedings of the IEEE Ultrasonics Symposium. IEEE; 1999. p. 501–4
34. 34. Boulder, Chapter 2: Semiconductor Fundamentals. August 2007
35. 35. Si F. Lecture 5 : Intrinsic Carrier concentration in intrinsic Si Carrier concentration in intrinsic semicon-. 2(2):1–5
36. 36. Diakite YI, Traore SD, Malozovsky Y, Khamala B, Franklin L, Bagayoko D. Accurate Electronic, Transport, and Bulk Properties of Gallium Arsenide (GaAs)
37. 37. Iskakova, Kulpash, Rif Akhmaltdinov, and Aisara Amanova. “About the energy levels of GaAs.” Journal of Physics: Conference Series (см. в книгах). Vol. 510. No. 1. Institute of Physics and IOP Publishing Limited, 2014
38. 38. Spirkoska D, Arbiol J, Gustafsson A, Conesa-Boj S, Glas F, Zardo I, et al. Structural and optical properties of high quality zinc-blende/wurtzite GaAs hetero-nanowires
39. 39. Iskakova K, Akhmaltdinov R, Amanova A. About the energy levels of GaAs. J Phys Conf Ser. 2014;510(1)
40. 40. Ashby, C., Baca, A. and Institution of Electrical Engineers., 2005. Fabrication Of Gaas Devices (EMIS Processing Series ; No. 6). Institution of Engineering and Technology - IET
41. 41. Pearsall TP. Indium Gallium Arsenide Phosphide. In: Encyclopedia of Materials: Science and Technology. Elsevier; 2001. p. 4048–6
42. 42. Dilli Z. Intrinsic and Extrinsic Semiconductors , Fermi-Dirac Distribution Function , the Fermi level and carrier concentrations Review : Charge Carriers in Semiconductors. Enee. 2009;313:1–8
43. 43. Nugroho MB. Semoconductor Bandstructure. J Chem Inf Model. 2013; 53(9):1689–99
44. 44. Sharmin M, Choudhury S, Akhtar N, Begum T. Optical and Transport Properties of p-Type GaAs. J Bangladesh Acad Sci. 2012 Jun 17;36(1):97–107
45. 45. Požela J, Reklaitis A. Electron transport properties in GaAs at high electric fields. Solid State Electron. 1980 Sep 1;23(9):927–33
46. 46. Guen-Bouazza A, Sayah C, Bouazza B, Chabane-Sari NE. Comparison of electron transport properties in submicrometer InAs, InP and GaAs n+−i-n+ diode using ensemble Monte Carlo simulation. J Mater Environ Sci. 2014;5(4):1238–43
47. 47. Požela J, Reklaitis A. Electron transport properties in GaAs at high electric fields. Solid State Electron. 1980 Sep 1;23(9):927–33
48. 48. Electronic Materials, Devices, and Fabrication (Prof. S. Parasuraman, IIT Madras): Lecture 02 - Introduction to Semiconductors
49. 49. Price GL. Gallium Arsenide and Related Compounds. Met forum. 1984;7(3):171–86
50. 50. Leds O. Lecture 16 : Light emitting diodes. :1–13
51. 51. Nguyen RH. Gallium arsenide. IEEE Potentials. 1999 Dec;17(5):33–5
52. 52. Das C, Begum J, Begum T, Choudhury S. EFFECT OF THICKNESS ON THE OPTICAL PROPERTIES OF GaAs THIN FILMS. Vol. 37, Journal of Bangladesh Academy of Sciences. 2013
53. 53. Taheri A, Davoodi M, Setayeshi S. Investigation of electron mobility in GaAs-based devices using genetic algorithm. COMPEL - Int J Comput Math Electr Electron Eng. 2012;31(2):604–18
54. 54. Anua NN, Ahmed R, Shaari A, Ul Haq B, Binti Mohamad M. DFT investigations of the optical properties of gallium arsenide. In: Advanced Materials Research [Internet]. Trans Tech Publications Ltd; 2014. p. 429–38
55. 55. Tanasa C, Lee J, Montoya J, Singh B, Tanasa C. “ Real ” Semiconductor Project GaAs Part 3. 2001;1–16
56. 56. Buonanno PR, Astronomico O, Cnr IFAC, Panciatichi V, Vanni PP. AT T I D E L L A « F ONDA Z ION E GI O RG IO RO NCHI ». 2012;(January)
57. 57. Al-ammar KHB, Hashim FS, Jappor. Structural and electronic properties of gallium arsenide crystal using INDO method. :1–16
58. 58. Tanasa C, Lee J, Montoya J, Singh B, Tanasa C. “ Real ” Semiconductor Project GaAs Part 1. 2001;1–16
59. 59. Surfaces S. GaAs Heterostructures and 2D electron gas. Screening. :8–16
60. 60. Brozel M. (2006) Gallium Arsenide. In: Kasap S., Capper P. (eds) Springer Handbook of Electronic and Photonic Materials. Springer Handbooks. Springer, Boston, MA
61. 61. Agarwal U, Chandra S, Kumar V. Structural , Electronic and Elastic Properties of zincblende III-Arsenide Binary Compounds : First-Principles Study. 0(1)
62. 62. Pluengphon P, Bovornratanaraks T. Structural and mechanical properties of GaAs under pressure up to 200 GPa. Solid State Commun 2014;195:26–30
63. 63. Güler E, Güler M. Phase transition and elasticity of gallium arsenide under pressure. Mater Res. 2014 Sep 1;17(5):1268–72. 51. Flannery CM, Chilla E, Semenov S, Froehlich HJ. Elastic properties of GaAs obtained by inversion of laser-generated surface acoustic wave measurements. In: Proceedings of the IEEE Ultrasonics Symposium. IEEE; 1999. p. 501–4
64. 64. Boulder, Chapter 2: Semiconductor Fundamentals. August 2007
65. 65. Si F. Lecture 5 : Intrinsic Carrier concentration in intrinsic Si Carrier concentration in intrinsic semicon-. 2(2):1–5
66. 66. Surfaces S. GaAs Heterostructures and 2D electron gas. Screening. :8–16
67. 67. Spirkoska D, Arbiol J, Gustafsson A, Conesa-Boj S, Glas F, Zardo I, et al. Structural and optical properties of high quality zinc-blende/wurtzite GaAs hetero-nanowires
68. 68. Iskakova K, Akhmaltdinov R, Amanova A. About the energy levels of GaAs. J Phys Conf Ser. 2014;510(1)
69. 69. Kayali S. I. GaAs Material Properties. Kabita K, Maibam J, Sharma BI, Brojen Singh RK, Thapa RK. Density functional theory study on pressure induced structural transformation, elastic properties and electronic structure of gallium arsenide (GaAs) . Vol. 8, International Journal of Innovation and Applied Studies. 2014
70. 70. Maurer RH, Chao K, Brent Bargeron C, Benson RC. RELIABILITY OF GALLIUM ARSENIDE DEVICES
71. 71. Pandey BP. Electronic and Optical Properties of GaAs Armchair Nanoribbons: DFT Approach. Vol. 11, International Journal of Nanoelectronics and Materials. 2018

Submitted: 17 August 2020 Reviewed: 20 October 2020 Published: 06 November 2020

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