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Theoretical Study of UV Surface Waves in AlAs and AlN

Arjun Mishra, Daya Shanker

Abstract


Surface waves excited at the interface between polar semiconductor surface and a dielectric when electromagnetic waves of appropriate frequency are incident on it. When the incident electromagnetic energy in the form of photons is absorbed, these surface excitations generate. They are of different kinds such as plasmon, phonon, exciton etc. Plasmon is the quanta of valence electron oscillation; phonon is the quanta of lattice vibration and exciton is the quanta of electron-hole pair oscillation. When a photon is coupled with any of these excitations, polariton waves excite. So, they are also different types such as plasmon-polariton, phonon-polariton, exciton-polariton etc. Dispersion relation, obtained from Maxwell equations, helps to study these excitations. This relation gives frequency dependent dielectric function ε(ω) and for the existence of surface waves, this dielectric function ε(ω) must be negative. Here, planar interface between semiconductors (Aluminium Arsenide (AlAs) and Aluminium Nitride (AlN)) and vacuum is taken for the study of coupled optical phonon-plasmon surface oscillations. The ratio between incident frequency (ω) and plasmon frequency (ωp) is calculated for different values of dielectric function. Two coupling frequency modes(ω/ωp)+and (ω/ωp) are obtained. For AluminiumArsenide (AlAs) and Aluminium Nitride (AlN), this surface wave exists when (ω/ωp)+less than 0.35 and (ω/ωp)+less than 0.46 respectively; as for this range, the dielectric function remains negative. These modes are obtained in the ultraviolet (UV) region (1016 Hz). The other (ω/ωp) mode remains nearly constant with values 0.0033 and 0.0036 for AlAs and AlN respectively and found in Infrared (IR) region (1013 Hz). Study of these and other new materials with other geometries such as cylindrical, spherical etc. can give promising results. Nanotubes are cylindrical in shapes, so this method is useful to analyse them. The surface modes in different frequency ranges have great role and these findings have importance in the synthesis of modern sophisticated optical devices (light emitting diodes: LEDs, sensors, photodetectors etc.) and useful for different technologies.


Keywords


Dispersion relation, Dielectric function, Plasmons, Phonons, Semiconductor.

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References


Kittel C. Introduction to solid state physics. John Wiley & Sons, Inc; 2005.

Dhibi A, Khemiri M, Oumezzine M. Theoretical Study of the Doping Effects of n-type and p-type Silicon on the Surface Plasmon Resonance Using a 2D Grating. Silicon. 2018 Nov; 10(6):

–41.

Tang WX, Zhang HC, Ma HF, Jiang WX, Cui TJ. Concept, theory, design, and applications of spoof surface plasmon polaritons at microwave frequencies. Adv Opt Mater. 2019 Jan; 7(1):

Ha DT, Thuy DT, Hoa VT, Van TT, Viet NA. On the theory of three types of polaritons (phonon,exciton and plasmon polaritons). J Phys: Conf Ser. 2017 Jun 1; 865(1): 012007. IOP Publishing.

Afinogenov BI, Kopylova DS, Abrashitova KA, Bessonov VO, Anisimov AS, Dyakov SA, Gippius NA, Gladush YG, Fedyanin AA, Nasibulin AG. Midinfrared surface plasmons in carbon nanotube

plasmonic metasurface. Phys Rev Appl. 2018 Feb 26; 9(2): 024027.

Wang Y, Cui Z, Zhu D, Zhang X, Qian L. Tailoring terahertz surface plasmon wave through free- standing multi-walled carbon nanotubes metasurface. Opt Express. 2018 Jun 11; 26(12): 15343–52.

Eldlio M, Che F, Cada M. Drude-Lorentz model of semiconductor optical plasmons. In IAENGTransactions on Engineering Technologies: Special Issue of the World Congress on Engineering

and Computer Science. 2014; 41–49. Springer Netherlands.

Srivastava KS, Tandon A. Dispersion relation for coupled surface plasmon and surface optical-phonon waves in polar semiconductors for some finite geometries. Phys Rev B. 1989 Feb 15; 39(6):3885.

Aron A, Singh RK. Effects of Electromagnetic Waves on the Low Pass Filter Characteristics. In 2022 IEEE 13th International Conference on Computing Communication and Networking Technologies (ICCCNT). 2022 Oct 3; 1–4.

Wallis RF, Brion JJ. Theory of surface plasmon-surface optical phonon interaction in polar semiconductors. Solid State Commun. 1971 Dec 1; 9(23): 2099–103.

Srivastava KS, Sinha A, Srivastava R, Tandon A. Interaction between two surface excitations in degenerate polar semiconductors. Phys Status Solidi (B) Basic Res. 1988 Mar 1; 146(1): 141–7.

Srivastava KS, Tandon A, Trivedi M, Fatima N. Surface plasmon-optical phonon dispersion relation for spherical polar semiconductors. Physica B: Condens Matter. 1989 Sep 1; 159(3):

–303.

Srivastava KS, Srivastava R, Sinha A, Tandon A, Nigam AN. Interaction of magnetoplasmons with optical phonons in polar semiconductors. Phys Rev B. 1988 Jul 15; 38(2): 1357.

Strelniker YM, Bergman DJ. Itinerant versus localized plasmons in an assembly of metal-dielectric parallel flat slabs in the presence of a perpendicular magnetic field: Faraday and magneto-optical

Kerr effects. Phys Rev B. 2021 May 3; 103(20): 205302.

Leinonen A, Saastamoinen K, Pesonen H, Wu G, Visser TD, Turunen J, Friberg AT. Polarization modulation by surface plasmons in Young's double-slit setup. Phys Rev A. 2021 Oct 6; 104(4):

Sun Z, Basov DN, Fogler MM. Graphene as a source of entangled plasmons. Phys Rev Res. 2022 Jun 13; 4(2): 023208.

Stozharov VM. Surface Plasmons Excited by X-rays in the Surface Layers of Solids. Solids. 2022 Mar 1; 3(1): 122–46.

Liu C, Bai Y, Zhou J, Zhao Q, Qiao L, Liu C, Bai Y, Zhou J, Zhao Q, Qiao L. A review of graphene plasmons and its combination with metasurface. J Korean Ceram Soc. 2017 Sep 29; 54(5): 349–65.

García MA. Surface plasmons in metallic nanoparticles: fundamentals and applications. J Phys D: Appl Phys. 2011 Jun 24; 44(28): 283001.

Afinogenov BI, Kopylova DS, Abrashitova KA, Bessonov VO, Anisimov AS, Dyakov SA, Gippius NA, Gladush YG, Fedyanin AA, Nasibulin AG. Midinfrared surface plasmons in carbon nanotube plasmonic metasurface. Phys Rev Appl. 2018 Feb 26; 9(2): 024027.

Wang Y, Cui Z, Zhu D, Zhang X, Qian L. Tailoring terahertz surface plasmon wave through free-standing multi-walled carbon nanotubes metasurface. Opt Express. 2018 Jun 11; 26(12):15343–52.

Afanas’ev SA, Zolotovskii IO, Kadochkin AS, Moiseev SG, Svetukhin VV, Pavlov AA. Continuous-wave laser generation of slow THz surface plasmons in an array of single-walled carbon nanotubes. Quantum Electron. 2018 Sep 1; 48(9): 849.

Shi Z, Hong X, Bechtel HA, Zeng B, Martin MC, Watanabe K, Taniguchi T, Shen YR, Wang F.Observation of a Luttinger-liquid plasmon in metallic single-walled carbon nanotubes. NatPhotonics. 2015 Aug; 9(8): 515–9.

Shuba MV, Yuko DI, Kuzhir PP, Maksimenko SA, Chigir GG, Pyatlitski AN, Sedelnikova OV, Okotrub AV, Lambin P. Localized plasmon resonance in boron-doped multiwalled carbon

nanotubes. Phys Rev B. 2018 May 16; 97(20): 205427.

Martín-Moreno L, de Abajo FJ, García-Vidal FJ. Ultraefficient coupling of a quantum emitter to the tunable guided plasmons of a carbon nanotube. Phys Rev Lett. 2015 Oct 20; 115(17): 173601.

Yanagi K, Okada R, Ichinose Y, Yomogida Y, Katsutani F, Gao W, Kono J. Intersubband plasmons in the quantum limit in gated and aligned carbon nanotubes. Nat Commun. 2018 Mar 16; 9(1):1121.

Ho PH, Farmer DB, Tulevski GS, Han SJ, Bishop DM, Gignac LM, Bucchignano J, Avouris P, Falk AL. Intrinsically ultrastrong plasmon–exciton interactions in crystallized films of carbon nanotubes. Proc Natl Acad Sci. 2018 Dec 11; 115(50): 12662–7.

Xu Y, Ang YS, Wu L, Ang LK. High sensitivity surface plasmon resonance sensor based on two- dimensional MXene and transition metal dichalcogenide: a theoretical study. Nanomaterials. 2019Jan 29; 9(2): 165.

Wang X, Pang Z, Yang H, Qi Y. Theoretical study of subwavelength circular grating fabrication based on continuously exposed surface plasmon interference lithography. Results Phys. 2019 Sep

; 14: 102446.

Zhu S, Fan C, Ding P, Liang E, Hou H, Wu Y. Theoretical investigation of a plasmonic substrate with multi-resonance for surface enhanced hyper-Raman scattering. Sci Rep. 2018 Aug 8; 8(1):

Richard-Lacroix M, Deckert V. Direct molecular-level near-field plasmon and temperature assessment in a single plasmonic hotspot. Light Sci Appl. 2020 Mar 9; 9(1): 35.

Radziuk D, Moehwald H. Prospects for plasmonic hot spots in single molecule SERS towards the chemical imaging of live cells. Phys Chem Chem Phys. 2015; 17(33): 21072–93.

Madzharova F, Heiner Z, Kneipp J. Surface enhanced hyper-Raman scattering of the amino acids

tryptophan, histidine, phenylalanine, and tyrosine. J Phys Chem C. 2017 Jan 19; 121(2): 1235–42.

Wasserroth S, Heeg S, Mueller NS, Kusch P, Hübner U, Gaufrès E, Tang NY, Martel R, Vijayaraghavan A, Reich S. Resonant, plasmonic Raman enhancement of α-6t molecules encapsulated in carbon nanotubes. J Phys Chem C. 2019 Apr 2; 123(16): 10578–85.

Srivastava KS, Singh AK, Tandon A, Trivedi M, Fatima N. Filtering properties of polar semiconductors. Physica B: Condens Matter. 1989 Dec 1; 160(3): 347–51.

Kumar V, Sastry BS. Heat of formation of ternary chalcopyrite semiconductors. J Phys Chem Solids. 2005 Jan 1; 66(1): 99–102.

Massa NE, Mitra SS, Vetelino JF. Lattice dynamics of mixed alkali halides. I. Negative-ionsubstitution. Phys Rev B. 1982 Oct 15; 26(8): 4579.

Massa NE, Vetelino JF, Mitra SS. Lattice dynamics of mixed alkali halides. II. Positive-ionsubstitution. Phys Rev B. 1982 Oct 15; 26(8): 4606.




DOI: https://doi.org/10.37591/rrjophy.v12i1.3562

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