• Title/Summary/Keyword: magnetic semiconductor

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Magneto-optical Measurements of Semiconductor Quantum Structures in Pulsed-magnetic Fields

  • Kim, Yongmin
    • Applied Science and Convergence Technology
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    • v.23 no.1
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    • pp.1-13
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    • 2014
  • Semiconductor quantum structures are often characterized by their energy gaps which are modified by the quantum size effect. Energy levels in semiconductors can be realized by optical transitions within confined structures. Photoluminescence spectroscopy in magnetic fields at low temperatures has proved to be a powerful technique for investigating the electronic states of quantum semiconductor heterostructures and offers a complimentary tool to electrical transport studies. In this review, we examine comprehensive investigations of magneto-excitonic and Landau transitions in a large variety of undoped and doped quantum-well structures. Strong magnetic fields change the diamagnetic energy shift of free excitons from quadratic to linear in B in undoped single quantum well samples. Two-dimensional electron gas induced by modulation doping shows pronounce quantum oscillations in integer quantum Hall regime and discontinuous transition at ${\nu}=1$. Such discontinuous transition can be explained as the formation of spin waves or Skyrmions.

Magnetic Properties of Cu-doped AlN Semiconductor (AlN 반도체와 Cu의 도핑 농도에 대한 자성)

  • Kang, Byung-Sub;Lee, Haeng-Ki
    • Journal of the Semiconductor & Display Technology
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    • v.9 no.3
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    • pp.1-4
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    • 2010
  • First-principles calculations based on spin density functional theory are performed to study the spin-resolved electronic properties of AlN doped with a Cu concentration of 6.25%-18.75%. The ferromagnetic state is more energetically favorable state than the antiferromagnetic state or the nonmagnetic state. For $Al_{0.9375}Cu_{0.0625}N$, a global magnetic moment of 1.26 mB per supercell, with a localized magnetic moment of 0.75 $m_B$ per Cu atom is found. The magnetic moment is reduced due to an increase in the number of Cu atoms occupying adjacent cation lattice position. For $Al_{0.8125}Cu_{0.1875}N$, the magnetism of the supercell disappears by the interaction of the neighboring Cu atoms. The nonmagnetic to ferromagnetic phase transition is found to occur at this Cu concentration. The range of concentrations that are spin-polarized should be restricted within very narrow.

Structural, Electrical and Magnetic Properties of Wide Bandgap Diluted Magnetic Semiconductor CuAl1-xMnxO2 Ceramics (널은 띠간격 묽은 자성반도체 CuAl1-xMnxO2 세라믹스의 구조 및 전자기 특성)

  • Ji Sung Hwa;Kim Hyojin
    • Korean Journal of Materials Research
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    • v.14 no.8
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    • pp.595-599
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    • 2004
  • We investigated the structural, electrical and magnetic properties of Mn-doped $CuAlO_2$ delafossite ceramics ($CuAl_{1-x}Mn_{x}O_2,\;0\le\;x\;\le0.05$), synthesized by solid-state reaction method in an air atmosphere at a sintering temperature of $1150^{\circ}C$. The solubility limit of Mn ions in delafossite $CuAlO_2$ was found to be as low as about 3 $mol\%$. Positive Hall coefficient and the temperature dependence of conductivity established that non-doped $CuAlO_2$ ceramic is a variable-range hopping p-type semiconductor. It was found that the Mn-doping in $CuAlO_2$ rapidly reduced the hole concentration and conductivity, indicating compensation of free holes. The analysis of the magnetization data provided an evidence that antiferromagnetic superexchange interaction is the dominant mechanism of the exchange coupling between Mn ions in $CuAl_{1-x}Mn_{x}O$ alloy, leading to an almost paramagnetic behavior in this alloy.

MAGNETOTRANSPORT IN AN N-TYPE DILUTED MAGNETIC SEMICONDUCTOR: (Ga,Mn)N

  • Lee, K. I.;Lee, J. M.;J. Y. Chang;S. H. Han;Lee, W. Y.;M. H. Ham;J. M. Myoung
    • Proceedings of the Korean Magnestics Society Conference
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    • 2002.12a
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    • pp.148-149
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    • 2002
  • In recent years, semiconductor spintronics has been rapidly developing due to potential device applications, in which the spin of charge carriers (electrons or holes) provides novel functionalities to carry signals and process information. Diluted magnetic semiconductors (DMSs) are well known to exhibit intriguing properties such as carrier-mediated ferromagnetism and spin-dependent transport resulting from the coupling between the charge transport states and the magnetic moments (spin) [1-3]. (omitted)

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MRAM Technology for High Density Memory Application

  • Kim, Chang-Shuk;Jang, In-Woo;Lee, Kye-Nam;Lee, Seaung-Suk;Park, Sung-Hyung;Park, Gun-Sook;Ban, Geun-Do;Park, Young-Jin
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.2 no.3
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    • pp.185-196
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    • 2002
  • MRAM(magnetic random access memory) is a promising candidate for a universal memory with non-volatile, fast operation speed and low power consumption. The simplest architecture of MRAM cell is a combination of MTJ(magnetic tunnel junction) as a data storage part and MOS transistor as a data selection part. This article will review the general development status of MRAM and discuss the issues. The key issues of MRAM technology as a future memory candidate are resistance control and low current operation for small enough device size. Switching issues are controllable with a choice of appropriate shape and fine patterning process. The control of fabrication is rather important to realize an actual memory device for MRAM technology.

Half-metallic Ferromagnetism for Mn-doped Chalcopyrite (Al,Ga)As Semiconductor (Chalcopyrite (Al,Ga)As 반도체와 Mn의 반금속 강자성)

  • Kang, B.S.;Song, K.M.
    • Journal of the Semiconductor & Display Technology
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    • v.19 no.3
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    • pp.49-54
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    • 2020
  • We studied the electronic and magnetic properties for the Mn-doped chalcopyrite (CH) AlAs, GaAs, and AlGaAs2 semiconductor by using the first-principles calculations. The chalcopyrite AlGaP2, AlGaAsP, and AlGaAs2 compounds have a semiconductor characters with a small band-gap. The interaction between Mn-3d and As-4p states at the Fermi level dominate rather than the other states. The ferromagnetic ordering of dopant Mn with high magnetic moment is induced due to the Mn(3d)-As(4p) strong coupling, which is attributed by the partially filled As-4p bands. The holes are mediated with keeping their 3d-electrons, therefore the ferromagnetic state is stabilized by this double-exchange mechanism. We noted that the ferromagnetic state with high magnetic moment is originated from the hybridized As(4p)-Mn(3d)-As(4p) interaction mediated by the holes-carrier.

A First Principles Study of Mn on AlGaP2 Semiconductor Surface (AlGaP2 반도체내와 표면의 Mn에 대한 제일원리 해석)

  • Kang, Byung Sub
    • Journal of the Semiconductor & Display Technology
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    • v.20 no.1
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    • pp.12-17
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    • 2021
  • The electronic and magnetic properties for Mn-adsorbed on the chalcopyrite (CH) AlGaP2 semiconductor are investigated by using first-principles FPLMTO method. The clean CH-AlGaP2 without adsorbed Mn is a p-type semiconductor with a direct band-gap. The Mn-adsorbed CH-AlGaP2 exhibits the ferromagnetic state. It is more energetically stable than the other magnetic ones. The interstitial site on P-terminated surface is more energetically favorable one than the Al/Ga-terminated surface, or the other adsorbing sites. In the case of Mn-adsorbed Al/Ga-terminated surface, it is induced a strong coupling between Mn-3d and neighboring P-3p electrons. The holes of partially unoccupied minority Mn-3d state and majority (or minority) Al-3p or P-3p state are induced. Thus a high magnetic moment of Mn is sustained by holes-mediated double-exchange coupling. It is noticeable that the semiconducting and half-metallic characteristics of CH-AlGaP2:Mn thin film is disappeared.

Ferromagnetic Properties in Diluted Magnetic Semiconductors (Al,Mn)N grown by PEMBE

  • Ham, Moon-Ho;Myoung, Jae-Min
    • Transactions on Electrical and Electronic Materials
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    • v.7 no.1
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    • pp.12-15
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    • 2006
  • We present the structural, magnetic, and electrical properties in the (Al,Mn)N films with various Mn concentrations grown by plasma-enhanced molecular beam epitaxy. X-ray diffraction analyses reveal that the (Al,Mn)N films have the wurtzite structure without secondary phases. All (Al,Mn)N films showed the ferromagnetic ordering. Particularly, ($Al_{1-x}Mn_{x}$)N film with x = 0.028 exhibited the highest magnetic moment per Mn atom at room temperature. Since all the films exhibit the insulating characteristics, the origin of ferromagnetism in (Al,Mn)N might be attributed to either indirect exchange interaction caused by virtual electron excitations from Mn acceptor level to the valence band within the samples or a percolation of bound magnetic polarons arisen from exchange interaction of localized carriers with magnetic impurities in a low carrier density regime.