• Title/Summary/Keyword: energy gap

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Introduction to research of atomically thin MoS2 and its electrical properties (2차원 MoS2 물질 기반의 전자소자 연구)

  • Lee, Takhee;Kim, Tae-Young;Cho, Kyungjune;Pak, Jinsu
    • Vacuum Magazine
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    • v.3 no.1
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    • pp.9-15
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    • 2016
  • Molybdenum disulfide ($MoS_2$), which has 0.65 nm-thick atomic layer, can be easily separated layer by layer due to weak van der Waals interactions in out-of-plane direction. ($MoS_2$), has a good potential in nanoelectronics, because it has high electrical mobility and On/Off ratio. Its band gap energy changes from indirect to direct band gap energy as it goes from bulk to monolayer. Therefore, atomically thin ($MoS_2$), is widely studied in academic and engineering fields. Here, we introduce the research of atomically thin $MoS_2$ and discuss the research directions.

Photoluminescence of Hexagonal Boron Nitride (h-BN) Film

  • Jin, Moon-Seog;Kim, Nam-Oh
    • Journal of Electrical Engineering and Technology
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    • v.5 no.4
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    • pp.637-639
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    • 2010
  • Hexagonal boron nitride (BN) films were prepared. The process involved, spraying BN powder-dispersed $H_3BO_4-BCl_3$-ethyl alcohol solution on quartz plates, and the drying off quartz plates before, and annealing at $1070^{\circ}C$ in a nitrogen atmosphere. The optical energy band gap of the BN films was 5.28 eV. Photoluminescence peaks with energies of 3.44, 3.16, 2.97, and 2.35 eV at 10 K were observed and analyzed. Accordingly, these have resulted from donor-acceptor pair recombinations.

Spin-polarized energy-gap opening in asymmetric bilayer graphene nanoribbons

  • Kim, Gyu-Bong;Ji, Seung-Hun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.442-442
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    • 2011
  • Electronic and magnetic properties of bilayer zigzag graphene nanoribbon (bZGNR) are studied using pseudopotential density functional method. The edge atoms in the top and bottom layers of bZGNR make a weak hybridization, which leads to electronic structures different from monolayer ZGNR. For asymmetric bZGNR, where the top and bottom layers have different widths, one edge is pinched by the interlayer bonding and the other sustains antiferromagnetic ordering. A small amount of charge transfer occurs from narrower to wider layer, producing spin-polarized electron and hole pockets. External electric field produces asymmetric energy-gap opening for each spin component, inducing half-metallicity in bZGNR.

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Effect of Ga, S Additions in CuInSe$_2$ for Solar Cell Applications

  • Kim, Kyoo-Ho
    • Journal of Surface Science and Engineering
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    • v.37 no.4
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    • pp.191-195
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    • 2004
  • Gallium or sulphur additions in $CuInSe_2$ were prepared using RF magnetron sputtering and pulsed laser deposition respectively. All of the observed thin films shows a chalcopyrite structure with the S and Ga addition increases the favourable (112) peak. The optical absorption coefficients were slightly decreased. The energy band gap of films could be shifted from 1.04 to 1.68 eV by adjusting the mole ratio of S/(S+Se) and Ga/(In+Ga). It is possible to obtain the optimum energy band gap by adding S or Ga solute at a certain ratio in favour of Se and In respectively. It is also necessary to control the ratio of Ga and S additions and to retain a certain portion of In and Se to provide better properties of thin films.

Optical Properties of Semiconductors Depending on the Contact Characteristic Between Different Groups (이종 물질의 접합계면에 의한 반도체 물질의 광학적 특성)

  • Oh, Teresa;Nho, Jong Ku
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.27 no.2
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    • pp.71-75
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    • 2014
  • To observe the optical characteristic of oxide semiconductor depending on the degree of bonding structures, SiOC, ZnO and IGZO were prepared by the RF magnetron sputter system and chemical vapor deposition. Generally, crystal ZnO, amorphous SiOC and IGZO changed the optical characteristics in according to the electro-chemical behavior due to the oxygen vacancy at an interface between different groups. Transmittance of SiOC and IGZO with amorphous structures was higher than that of ZnO with crystal structure, because of lowering the carrier concentration due to the recombination of electron and holes carriers as oxygen vacancies. Besides, the energy gap of amorphous SiOC and IGZO was higher than the energy gap of crystal ZnO. The diffusion mobility of holes is higher than the drift mobility of electrons.

Synthesis, Optical and Electrical Studies of Nonlinear Optical Crystal: L-Arginine Semi-oxalate

  • Vasudevan, P.;Sankar, S.;Jayaraman, D.
    • Bulletin of the Korean Chemical Society
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    • v.34 no.1
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    • pp.128-132
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    • 2013
  • L-Arginine semi-oxalate (LASO) single crystal has been grown by solution growth technique at room temperature. The crystal structure and lattice parameters were determined for the grown crystal by single crystal X-ray diffraction studies. Photoluminescence studies confirm the violet fluorescence emission peak at 395 nm. Optical constants like band gap, refractive index, reflectance, extinction coefficient and electric susceptibility were determined from UV-VIS-NIR spectrum. The dielectric constant, dielectric loss and ac conductivity of the compound were calculated at different temperatures and frequencies to analyze the electrical properties. The solid state parameters such as plasma energy, Penn gap, Fermi energy and polarizability were calculated to analyze second harmonic generation (SHG). Nonlinear optical property was discussed to confirm the SHG efficiency of the grown crystal.

Quantum dot and their applications (양자점과 응용기술)

  • Son, Dong Ick
    • Vacuum Magazine
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    • v.4 no.4
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    • pp.4-13
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    • 2017
  • Quantum structures containing nanoparticles have attracted much attention because of their promising potential applications in electronic and optoelectronic devices operating at lower currents and higher temperatures. The quantum dot is a particle of matter so small that the addition or removal of an electron changes its properties in some useful way. The Quantum dots typically have dimensions measured in nanometers, where one nanometer is 10-9 meter or a millionth of a millimeter. The emission and absorption spectra corresponding to the energy band gap of the quantum dot is governed by quantum confinement principles in an infinite square well potential. The energy band gap increases with a decrease in size of the quantum dot. In this review paper, we will discuss the quantum dot and their application.

The Dependence of Electrical Conductivity of Cupric Oxide on Temperature (산화동에 있어 온도변화에 의한 전기전도도에 관한 연구)

  • 안영필;이희동
    • Journal of the Korean Ceramic Society
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    • v.20 no.2
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    • pp.161-165
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    • 1983
  • We studied the dependence of electrical conduction mechanism of Cupric Oxide on temperature and measured the specific resistivity of sintered specimen from $600^{\circ}C$ to 90$0^{\circ}C$ . We considered the relations between electrical conducti-vityand temperature with reheating the sintered specimen. X-Ray diffraction patterns showed that lattice parameters of cupric oxide increased above 20$0^{\circ}C$. Cupric oxide had nostoichiometric compositions$(CuO_{1+x})$ owing to the excess oxygen and showed hole conduction with energy gap of 0.15eV below $650^{\circ}C$$\pm$1$0^{\circ}C$ Above $650^{\circ}C$$\pm$1$0^{\circ}C$ cupic oxide had the stoichiometric composition and showed electron-hole conduction owing to the intrinsic ionization with energy gap of 1.04V.

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Growth and optical properties of undoped and Co-doped CdS single crystals (CdS 및 $CdS:Co^{2+}$ 단결정의 성장과 광학적 특성)

  • Kim, N.O.;Bang, T.H.;Hyun, S.C.;Park, K.H.;Park, H.;Oh, S.K.
    • Proceedings of the KIEE Conference
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    • 2002.06a
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    • pp.94-97
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    • 2002
  • CdS and $CdS:Co^{2+}$ single crystals were grown by CTR method using iodine as transport material. The grown single crystals have defect chalcopyrite structure with direct band gap. The optical energy band gap was decreased according to add of Co-impurity. We can observed the Co-impurity optical absorption peaks assigned to the $Co^{2+}$ ion sited at the $T_d$ symmetry lattice and we consider that they were attributed to the electron transitions between energy levels of ions.

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Crystal Growth of $Cd_4SnSe_6:Co^{2+}$ Single Crystals ($Cd_4SnSe_6:Co^{2+}$ 단결정의 성장)

  • Kim, D.T.;Song, M.J.;Kim, H.G.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2005.07a
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    • pp.607-608
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    • 2005
  • In this paper, author describe the undoped and $Co^{2+}$(0.5mole%) doped $Cd_4SnSe_6$ single crystals were grown by the chemical transport reaction(CTR) method. The grown single crystals crystallize in the monoclinic structure of space group Cc and have the direct band gap structure. The energy gaps of them are 1.68 eV for $Cd_4SnSe_6$ and 1.50 eV for $Cd_4SnSe_6:Co^{2+}$ at 300K respectively.

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