1984
DOI: 10.1016/0022-2313(84)90331-4
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Emission of free and bound excitons in GaSe and InSe crystals in direct and indirect transition region

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Cited by 6 publications
(2 citation statements)
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“…The slit spectral width of monochromator did not exceed 0.2 meV at T = 5 K and 0.5 meV at T = 300 K. As it can be seen in Fig. 7d, at Т = 5 K the PL spectrum of GaSe crystal consists of lines corresponding to radiation of the free excitons ( = 587.8 nm, E exc = 2.108 eV) [12] as well as of excitons bound to stacking faults of crystalline layers, dislocation, and point defects. Besides, the PL spectrum in the range E < 2.050 eV (> 605.0 nm) contains several bands of a low intensity which, according to [4], are caused by transitions between the direct and indirect conduction bands and shallow acceptors in GaSe<RbNO 3 >.…”
Section: Photoluminescence Spectramentioning
confidence: 83%
“…The slit spectral width of monochromator did not exceed 0.2 meV at T = 5 K and 0.5 meV at T = 300 K. As it can be seen in Fig. 7d, at Т = 5 K the PL spectrum of GaSe crystal consists of lines corresponding to radiation of the free excitons ( = 587.8 nm, E exc = 2.108 eV) [12] as well as of excitons bound to stacking faults of crystalline layers, dislocation, and point defects. Besides, the PL spectrum in the range E < 2.050 eV (> 605.0 nm) contains several bands of a low intensity which, according to [4], are caused by transitions between the direct and indirect conduction bands and shallow acceptors in GaSe<RbNO 3 >.…”
Section: Photoluminescence Spectramentioning
confidence: 83%
“…Their mirrorlike surfaces are practically ideal with a normal parallel to the crystallographic C axis. A variety of electron transitions determines a complicated structure of PL spectra due to the presence of energy levels of various nature in the InSe energy gap [1][2][3][4][5][6][7][8]. So, ІnSe is an indirect semiconductor [9].…”
Section: Introductionmentioning
confidence: 99%