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Journal articles on the topic 'Cd(1-x)Mn(x)Te'

Author: Grafiati

Published: 28 May 2022

Last updated: 31 July 2025

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1

Masłowska, Aneta, Dominika M. Kochanowska, Adrian Sulich, et al. "Bridgman-Grown (Cd,Mn)Te and (Cd,Mn)(Te,Se): A Comparison of Suitability for X and Gamma Detectors." Sensors 24, no. 2 (2024): 345. http://dx.doi.org/10.3390/s24020345.

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This study explores the suitability of (Cd,Mn)Te and (Cd,Mn)(Te,Se) as room-temperature X-ray and gamma-ray detector materials, grown using the Bridgman method. The investigation compares their crystal structure, mechanical and optical properties, and radiation detection capabilities. Both crystals can yield large-area single crystal samples measuring approximately 30 × 30 mm2. In low-temperature photoluminescence analysis, both materials showed defect states, and annealing in cadmium vapors effectively eliminated donor–acceptor pair luminescence in (Cd,Mn)Te but not in (Cd,Mn)(Te,Se). Moreove

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2

GNANASEKAR, K., and K. NAVANEETHAKRISHNAN. "SPIN POLARON IN A QUANTUM DOT OF THE DILUTED MAGNETIC SEMICONDUCTORS." Modern Physics Letters B 18, no. 10 (2004): 419–26. http://dx.doi.org/10.1142/s0217984904006962.

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Theoretical investigations of spin polaron in a quantum dot in the "spin doping" superlattice systems Cd 1 - X in Mn X in Te/Cd 1 - X out Mn X out Te are presented. We estimated the donor ionization energy by variational technique and the spin polaronic shift using the mean field theory with modified Brillouin function. Our results show that significant enhancement of donor ionization energy and spin polaronic shift occur in a dot when compared to a quantum well, wire and bulk systems.

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3

Tan, Guo-Long, and Min Wang. "Ferromagnetism of Ternary Cd$_{\bf 1-}$$_{\bm x}$Mn $_{\bm x}$Te Nanocrystals." IEEE Transactions on Nanotechnology 11, no. 2 (2012): 236–38. http://dx.doi.org/10.1109/tnano.2010.2084098.

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4

Chen-Jia, Chen, Wang Xue-Zhong, Vittorio Bellani, and Angiolino Stella. "Studies of Spectroscopic Ellipsometry in Cd 1− x Mn x Te/CdTe Superlattices." Chinese Physics Letters 23, no. 1 (2006): 207–10. http://dx.doi.org/10.1088/0256-307x/23/1/060.

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5

Liu, Jizhou, Xuezhong Wang, Chenjia Chen, and Kejun Ma. "Magneto-Optical Bistability in Diluted Magnetic Semiconductor Cd 1-x Mn x Te." Chinese Physics Letters 10, no. 9 (1993): 562–65. http://dx.doi.org/10.1088/0256-307x/10/9/014.

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6

Kierzek-Pecold, E., W. Szymańska, and J. Ginter. "Long time effects in the spin glass Cd 1 −x Mn x Te." Journal of Magnetism and Magnetic Materials 50, no. 2 (1985): 243–46. http://dx.doi.org/10.1016/0304-8853(85)90189-1.

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7

PLOCH, D., J. CEBULSKI, and E. M. SHEREGII. "MAGNETOPHONON RESONANCE IN MnxCdyHg1-x-yTe." International Journal of Modern Physics B 21, no. 08n09 (2007): 1615–20. http://dx.doi.org/10.1142/s0217979207043300.

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The aim of this work is to analyze the band-structure parameters of Mn x Cd y Hg 1- x - y Te (MMCT) alloys by means of Magnetophonon Resonance (MPR) and to compare that obtained for Zn x Cd y Hg 1- x - y Te (ZMCT). MPR was observed for two samples of Mn x Cd y Hg 1- x - y Te (MMCT) (I- x =0.095 and y =0.09, II-0.04 and y =0.19). The measurements of MPR were performed in pulsed magnetic fields at different temperatures ranging from 77 K to 200 K. The several wide maxima are clearly visible on the experimental curves corresponding to four series of peaks. These series are related to three kinds

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8

ZHANG, Ji-Jun, Lin-Jun WANG, Jia-Hua MIN, et al. "Infrared transmission of Cd_1-x Mn_x Te crystal." JOURNAL OF INFRARED AND MILLIMETER WAVES 31, no. 2 (2012): 113–17. http://dx.doi.org/10.3724/sp.j.1010.2012.00113.

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9

Boudinet, P., and G. Bastard. "Acceptor-Bound Magnetic Polaron in CdTe-Cd 1− x Mn x Te Quantums Wells." Europhysics Letters (EPL) 20, no. 2 (1992): 149–53. http://dx.doi.org/10.1209/0295-5075/20/2/010.

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10

Kuroda, T., F. Minami, and S. Seto. "High-Density Excitons in a Diluted Magnetic Semiconductor: Cd 1 − x Mn x Te." Phase Transitions 75, no. 7-8 (2002): 1019–26. http://dx.doi.org/10.1080/01411590290034182.

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11

PETER, A. JOHN. "BINDING ENERGY OF ACCEPTORS IN SEMIMAGNETIC QUANTUM DOTS." International Journal of Nanoscience 05, no. 01 (2006): 173–81. http://dx.doi.org/10.1142/s0219581x06004164.

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The binding energies of shallow acceptors in Cd 1-x in Mn x in Te/ Cd 1-x out Mn x out Te quantum dots are calculated in the presence of external magnetic fields. Variational calculations are performed within effective mass approximation. The results show that the impurity binding energy (i) increases with the reduction in dot sizes, (ii) decreases with the magnetic field is increased for a given dot, and (iii) reaches a peak value as the dot radius decreases and then diminishes to a limiting value corresponding to the radius for which there are no bound states in the quantum dot. Spin polaron

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12

PETER, A. JOHN. "EFFECT OF MAGNETIC FIELDS ON BINDING ENERGY OF IMPURITY STATES IN A SEMIMAGNETIC PARABOLIC QUANTUM DOT." International Journal of Modern Physics B 21, no. 17 (2007): 3035–44. http://dx.doi.org/10.1142/s0217979207037363.

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Using a variational approach, the binding energy of shallow hydrogenic impurities in a semimagnetic parabolic quantum dot is calculated within the effective mass approximation. The binding energy is computed for Cd 1-x in Mn x in Te / Cd 1-x out Mn x out Te structures as a function of the dot size in an external magnetic field. The results show that the impurity binding energy (i) increases with the reduction in dot sizes (ii) decreases when the magnetic field is increased for a given dot and (iii) increases to a maximum value at 100 Å and then decreases as the size of the dot increases beyond

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13

Butler, M. A. "Wavelength and temperature dependence of the Faraday effect in Cd(1 − x)Mn(x)Te." Solid State Communications 62, no. 1 (1987): 45–47. http://dx.doi.org/10.1016/0038-1098(87)90081-0.

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14

Sawicki, M., T. Dietl, G. Karczewski, T. Wojtowicz, and Jacek Kossut. "Magnetic Characterization of MBE Grown Cd_1-xMn_xTe Structures." Materials Science Forum 182-184 (February 1995): 685–86. http://dx.doi.org/10.4028/www.scientific.net/msf.182-184.685.

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15

HWANG, Younghun, Youngho UM, and Hyo-yeol PARK*. "Studies of Spectroscopic Ellipsometry in Cd$_{1-x}$Mn$_x$Te(0.0 ≤ x ≤0.77) Single Crystals." New Physics: Sae Mulli 60, no. 7 (2010): 767–71. http://dx.doi.org/10.3938/npsm.60.767.

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16

Weili, Wang, Peng Songshi, Xing Qijiang, and Xu Xueyun. "Nonlinear absorption in Cd x Hg 1- x Te." Chinese Physics Letters 3, no. 3 (1986): 141–43. http://dx.doi.org/10.1088/0256-307x/3/3/012.

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17

Bundaleski, Nenad, Ivana Radisavljević, João Trigueiro, et al. "Surface composition of Cd 1–x Fe(Mn) x Te 1–y Se y systems exposed to air." Materials Chemistry and Physics 189 (March 2017): 35–43. http://dx.doi.org/10.1016/j.matchemphys.2016.12.029.

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18

SHARMA, ASHUTOSH, SWETALI NIMJE, AKSHAY SALIMATH, and BAHNIMAN GHOSH. "SPIN POLARIZED TRANSPORT IN Cd1-xMnxTe." SPIN 02, no. 04 (2012): 1250015. http://dx.doi.org/10.1142/s2010324712500154.

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Spin relaxation process is simulated for nanowires and 2-D channels composed of II–VI DMS materials, particularly for Cd 1-x Mn x Te , in our work. Our studies are focused on analyzing spin relaxation behavior at T = 1 K. Variations in spin relaxation length with applied field and concentration of Mn doping are calculated and plotted. Effect of one-magnon scattering process is significant due to magnetic nature of the materials and is demonstrated in this work.

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19

Radisavljević, Ivana, Nikola Novaković, Nebojša Romčević, et al. "Electronic aspects of formation and properties of local structures around Mn in Cd 1−x Mn x Te 1−y Se y." Materials Chemistry and Physics 167 (November 2015): 236–45. http://dx.doi.org/10.1016/j.matchemphys.2015.10.038.

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20

Zukowski, P. W. "Dielectric constant and ac conductivity of semi-insulating Cd[sub 1−x]Mn[sub x]Te semiconductors." Semiconductors 31, no. 6 (1997): 610. http://dx.doi.org/10.1134/1.1187227.

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21

Denysyuk, R. O. "Chemical treatment of Cd 1 вЂ“ x Mn x Te single crystals with H 2O2 вЂ“HIвЂ“citric acid aqueous solutions". Semiconductor Physics Quantum Electronics and Optoelectronics 17, № 1 (2014): 21–24. http://dx.doi.org/10.15407/spqeo17.01.021.

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22

YOUNGDALE, E. R., J. R. MEYER, F. J. BARTOLI, and C. A. HOFFMAN. "LARGE, WEAKLY SATURATING THIRD-ORDER NONLINEAR SUSCEPTIBILITIES IN SEMIMETALS AND NARROW-GAP SEMICONDUCTORS." Journal of Nonlinear Optical Physics & Materials 01, no. 03 (1992): 493–531. http://dx.doi.org/10.1142/s0218199192000248.

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We review recent experimental and theoretical work on optical nonlinearities in semimetals and narrow-gap semiconductors. A strong nonlinear response due to optical modulation of the free carrier susceptibility is seen to be a common feature of these materials, with large third-order nonlinear susceptibilities being reported for Hg 1−x Cd x Te , Hg 1−x Mn x Te , Hg-based superlattices, α- Sn 1−x Ge x, Pb 1−x Sn x Se , and Bi 1−x Sb x. Effects of differences in the various band structures are discussed for nonlinearities due to nonparabolicity, thermal carrier generation, and nonequilibrium car

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23

HIRAYAMA, Y., K. OTO, H. MINO, et al. "MAGNETO-PHOTOLUMINESCENCE STUDY AT A FRACTIONAL QUANTUM HALL REGIME OF CHARGED EXCITONS IN A DILUTE MAGNETIC SEMICONDUCTOR." International Journal of Modern Physics B 18, no. 27n29 (2004): 3821–24. http://dx.doi.org/10.1142/s0217979204027529.

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We have performed magneto-photoluminescence measurements on modulation doped n-type Cd 1-x Mn x Te / Cd 1-y Mg y Te single quantum wells. In low magnetic fields (the electrons filling factor ν>1), we observed several photoluminescence lines associated with spin-singlet and spin-triplet charged excitons. In high magnetic fields (ν<1), we observed only one of the spin-triplet charged excitons that are called as a bright type due to characteristic spin states of electrons and holes in dilute magnetic semiconductor quantum wells, where the photoluminescence intensity increased at a fractiona

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24

Barbot, J. F., G. Rivaud, H. Garem, et al. "Plastic behaviour of Cd x Hg1?x Te (0? x?1) crystals." Journal of Materials Science 25, no. 3 (1990): 1877–85. http://dx.doi.org/10.1007/bf01045400.

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25

Spasojevic, V., D. Rodic, A. Bajorek, and A. Szytula. "Magnetic susceptibility calculation of Cd 1-x Mn x S." Journal of Magnetism and Magnetic Materials 128, no. 3 (1993): 375–80. http://dx.doi.org/10.1016/0304-8853(93)90484-j.

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26

Scalbert, D. "Contribution of Spins Clusters to Magnetization Relaxation in Cd_1-xMn_xTe." Materials Science Forum 182-184 (February 1995): 451–54. http://dx.doi.org/10.4028/www.scientific.net/msf.182-184.451.

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27

Xue-chu, Shen, Ye Hong-juan, Kang Li-xue, and Tao Feng-xiang. "Acoustic local mode and TA band mode vibration for the mixed crystals Cd 1-x Mn x Te." Chinese Physics Letters 2, no. 5 (1985): 209–12. http://dx.doi.org/10.1088/0256-307x/2/5/005.

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28

Van, Cong Huynh. "34.151% (33.93%)-Maximal Efficiencies, obtained in CdTe(1-x)S(x), CdTe(1-x)Se(x)-Crystalline Alloy Junction Solar Cells at 300 K." European Journal of Applied Science, Engineering and Technology 2, no. 2 (2024): 125–49. https://doi.org/10.59324/ejaset.2024.2(2).10.

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In two new single n^+ (p^+)-p(n) X(x)-alloy junction solar cells at 300 K, [X(x)&equiv;CdTe_(1-x) S_x, CdTe_(1-x) Se_x],0≤x≤1, by basing on the same physical model-and-treatment method, as used in our recent works [1, 2], and also other works [3-11], some important results, obtained in the present work, are reported in the following.As noted in Tables 2.1, 3.1, 4.1 and 5.1, the dark carrier-minority saturation current density J_(oI(oII)) decreases slightly with increasing r_(d(a))-radius for given x, and decreases strongly with increasing x, for given r_(d(a))-radius. Further, as discuss

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29

Hamdani, F., T. Ruf, A. Waag, T. Litz, and G. Landwehr. "Carrier-Ion and Ion-Ion Exchange Interactions in Cd_1-xMn_xTe/Cd_1-yMg_yTe Heterostructures." Materials Science Forum 182-184 (February 1995): 751–54. http://dx.doi.org/10.4028/www.scientific.net/msf.182-184.751.

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30

H., SANO, YAMAGISHI A., KURITA J., MIZUTANI G., and SETO S. "OPTICAL SECOND HARMONIC SPECTROSCOPY OF Cd 1−x Zn x Te." Nonlinear Optics 29, no. 7-9 (2002): 421–26. http://dx.doi.org/10.1080/1058726021000044947.

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31

Butler, J. F., C. L. Lingren, and F. P. Doty. "Cd/sub 1-x/Zn/sub x/Te gamma ray detectors." IEEE Transactions on Nuclear Science 39, no. 4 (1992): 605–9. http://dx.doi.org/10.1109/23.159673.

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32

Sochinskii, Nikolai V., Sandra Rubio, José Luis Plaza, and Ernesto Diéguez. "Growth and structure of Cd 1–x Dy x Te crystals." Journal of Crystal Growth 449 (September 2016): 1–4. http://dx.doi.org/10.1016/j.jcrysgro.2016.05.006.

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33

Pietruczanis, J., W. Mac, Andrzej Twardowski, et al. "Magnetic Phase Diagram of Highly Concentrated Cd_1-xMn_xTe (0.4 < x < 1.0)." Materials Science Forum 182-184 (February 1995): 687–90. http://dx.doi.org/10.4028/www.scientific.net/msf.182-184.687.

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34

MASROUR, R., M. HAMEDOUN, and A. BENYOUSSEF. "CROSSOVER OF CRITICAL EXPONENTS INDUCED BY DILUTION VIA MONTE CARLO SIMULATIONS." International Journal of Modern Physics B 25, no. 32 (2011): 4573–85. http://dx.doi.org/10.1142/s0217979211059218.

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The crossover of dilution in the critical exponent associated with the thermodynamic properties in the magnetic materials via Monte Carlo simulations is observed. The obtained results of critical exponent associated with the magnetic susceptibility, specific heat and correlation length for the ZnCr 2x Al 2-2x S 4, Cd 1-y Cr 2-2x In y+2x Se 4 and Zn 1-x Mn x Te systems are comparable with those given by the experiment results.

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35

Afif, K., A. Benyoussef, and J. Diouri. "Auto-correlation Effects on the sp 3 -d Exchange Interaction in Cd 1- x Mn x Te/CdTe Multilayers." Chinese Physics Letters 19, no. 11 (2002): 1679–82. http://dx.doi.org/10.1088/0256-307x/19/11/333.

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36

Gentsar, P. O. "OPTICAL SPECTROSCOPY OF DETECTIVE HIGH RESISTANCE CdTe(111) MONOCRESISTORS AND SOLIDS Cd 1-x Zn x Te." Optoelektronìka ta napìvprovìdnikova tehnìka 58 (December 21, 2023): 128–35. http://dx.doi.org/10.15407/iopt.2023.58.128.

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Cadmium telluride is used for the manufacture of uncooled gamma radiation detectors, and solid solutions of Cd 1-x Zn x Te (x=0.1) are used for the manufacture of X-ray and gamma radiation detectors. The study of the effect of doping on the physical properties of semiconductors is relevant both for experimenters and for the theoretical substantiation of physical processes. This paper presents the results of the study of optical reflection spectra in the spectral range (0,2-1,7) . 10 -6 m and transmittance in the region of the fundamental optical transition E 0 of high-resistivity CdTe single c

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37

Luo, Pengfei, Li You, Jiong Yang, et al. "Effects of Mn substitution on thermoelectric properties of CuIn 1−x Mn x Te 2." Chinese Physics B 26, no. 9 (2017): 097201. http://dx.doi.org/10.1088/1674-1056/26/9/097201.

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38

Yong, Liang, Zheng Gouzhen, and Tang Dingyuan. "Acceptor levels in zero-gap Hg 1- x Cd x Te crystal." Chinese Physics Letters 3, no. 9 (1986): 425–28. http://dx.doi.org/10.1088/0256-307x/3/9/011.

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39

Tang, Ke, Jian Huang, Yuanxi Lu, et al. "Cd 1-x Zn x Te photodetectors with transparent conductive ZnO contacts." Applied Surface Science 433 (March 2018): 177–80. http://dx.doi.org/10.1016/j.apsusc.2017.10.023.

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40

Talwar, Devki N., and P. Becla. "Infrared and Raman characteristics of bulk Cd 1-x Mn x Te and (MnTe) m /(CdTe) n short period superlattices." Materials Letters 175 (July 2016): 279–83. http://dx.doi.org/10.1016/j.matlet.2016.04.056.

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41

Li, S. M., J. Q. Li, L. Yang, F. S. Liu, W. Q. Ao, and Y. Li. "Phases and thermoelectric properties in stoichiometric Sn 1−x Mn x Te and non-stoichiometric Sn 1−y Mn 1.1y Te alloys." Materials & Design 108 (October 2016): 51–59. http://dx.doi.org/10.1016/j.matdes.2016.06.084.

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42

Van, Cong Huynh. "34.375% (33.72%)-Maximal Efficiencies, obtained in CdSe(1-x)S(x), CdSe(1-x)Te(x)-Crystalline Alloy Junction Solar Cells at 300 K." European Journal of Applied Science, Engineering and Technology 2, no. 2 (2024): 150–74. https://doi.org/10.59324/ejaset.2024.2(2).11.

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In two new single n+(p+)−p(n) X(x)-alloy junction solar cells at 300 K, [X(x)&equiv;CdSe<sub>1−x</sub>S<sub>x</sub>, CdSe<sub>1−x</sub>Te<sub>x</sub>], 0≤x≤1, by basing on the same physical model-and-treatment method, as used in our recent works [1, 2], and also other works [3-6], some important results, obtained in the present work, are reported in the following.As noted in Tables 2.1, 3.1, 4.1 and 5.1, the dark carrier-minority saturation current density J<sub>oI(oII)</sub> decreases slightly with increasing r<sub>d(a)</sub>-radius for given x, and decreases stro

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43

JAYAM, Sr GERARDIN, and K. NAVANEETHAKRISHNAN. "OPTICAL PROPERTIES OF ACCEPTORS IN SEMIMAGNETIC QUANTUM WELL SYSTEMS." International Journal of Modern Physics B 16, no. 25 (2002): 3737–57. http://dx.doi.org/10.1142/s021797920201302x.

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The binding energy of a shallow acceptor in an isolated quantum well of the CdTe / Cd 1-x Mn x Te system has been investigated in an external magnetic field, assuming an empirical relationship between the barrier height and the magnetic field. Photoionization cross-sections for different magnetic fields have been estimated. Taking into account the confined phonons in the electron-phonon interaction, carrier capture times for various magnetic fields and different hydrostatic pressures have been computed. The results obtained are discussed in the light of the existing literature.

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44

Zerroug, S., A. Gueddim, and N. Bouarissa. "Composition dependence of fundamental properties of $$\hbox {Cd}_{\mathrm{1-x}}\hbox {Co}_\mathrm{x}$$ Cd 1 - x Co x Te magnetic semiconductor alloys." Journal of Computational Electronics 15, no. 2 (2016): 473–78. http://dx.doi.org/10.1007/s10825-016-0802-9.

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45

Duric, Z. G., and V. B. Jovic. "Epitaxial Growth of Hg_1-xCd_xTe." Materials Science Forum 214 (May 1996): 57–64. http://dx.doi.org/10.4028/www.scientific.net/msf.214.57.

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46

Шаров, М. К. "Тепловое расширение кристаллов Pb-=SUB=-1-x-=/SUB=-Cd-=SUB=-x-=/SUB=-Te". Физика и техника полупроводников 55, № 12 (2021): 1216. http://dx.doi.org/10.21883/ftp.2021.12.51708.9715.

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The values of the lattice period and the linear coefficient of thermal expansion (alfa) of Pb1-xCdxTe solid solutions are determined depending on the cadmium content and temperature using high-temperature X-ray diffractometry. Аn increase in the concentration of cadmium in Pb1-xCdxTe in the range x = 0.02–0.08 leads to a significant increase in the linear coefficient of thermal expansion. A change in temperature range T = 293–673 K leads to decrease in the linear coefficient of thermal expansion. Besides, an increase in temperature does not affect the value alfa of the undoped PbTe in the indi

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47

Leech, P. W., E. Stumpf, N. Petkovic, and L. W. Cahill. "Hg/sub 1-x/Cd/sub x/Te metal-semiconductor-metal (MSM) photodetectors." IEEE Transactions on Electron Devices 40, no. 8 (1993): 1364–70. http://dx.doi.org/10.1109/16.223693.

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48

Leontiadou, Marina A., Ali Al-Otaify, Stephen V. Kershaw, et al. "Ultrafast Exciton Dynamics in Cd x Hg (1 − x ) Te alloy Quantum Dots." Chemical Physics 469-470 (May 2016): 25–30. http://dx.doi.org/10.1016/j.chemphys.2016.02.003.

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49

Chen, X. T., H. Qiao, X. Y. Liu, and K. J. Yang. "Electrical properties of Hg 1− x Cd x Te by different etching techniques." Infrared Physics & Technology 73 (November 2015): 251–54. http://dx.doi.org/10.1016/j.infrared.2015.09.023.

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50

Kuroda, Satoshi, K. Kojima, K. Kobayashi, et al. "Magneto-Optical Study of Interface Diffusion in CdTe/Cd_1-xMn_xTe Multiple Quantum Wells." Materials Science Forum 182-184 (February 1995): 615–18. http://dx.doi.org/10.4028/www.scientific.net/msf.182-184.615.

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