Raman spectra of ordered vacancy compounds in the Cu-In-Se system
Raman spectra of ordered vacancy compounds (OVC) of CuIn 2 Se 3.5 and CuIn 3 Se 5 have been measured at room temperature. Similar nonpolarized Raman spectra are obtained for CuIn 2 Se 3.5 and CuIn 3 Se 5 . However, polarized Raman spectra are not available for CuIn 3 Se 5 because of its unfavorable...
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Published in | Japanese Journal of Applied Physics Vol. 36; no. 8B; pp. L1075 - L1077 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Tokyo
Japanese journal of applied physics
15.08.1997
|
Subjects | |
Online Access | Get full text |
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Summary: | Raman spectra of ordered vacancy compounds (OVC) of CuIn
2
Se
3.5
and CuIn
3
Se
5
have been measured at room temperature. Similar nonpolarized Raman spectra are obtained for CuIn
2
Se
3.5
and CuIn
3
Se
5
. However, polarized Raman spectra are not available for CuIn
3
Se
5
because of its unfavorable crystallinity. A signal at 154 cm
-1
is assigned to be Γ
1
mode of
D
2
d
symmetry, originating from the vibration of selenium atoms in the
x
-
y
(
a
-axes) plane. This signal corresponds to the signal at 178 cm
-1
for CuInSe
2
of chalcopyrite-type in the Cu-In-Se system. The lowering of Γ
1
mode frequency for the defect structure is attributed to looser-bound selenium atoms on account of vacancies in the cation sites. Signals assigned as Γ
3
mode are unexpectedly observed in the geometries allowing the longitudinal optical (LO) modes of Γ
4
and Γ
5
symmetries. The respective mode peaks are found to be more dispersive in frequency for CuIn
2
Se
3.5
than for CuInSe
2
. |
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ISSN: | 0021-4922 1347-4065 |
DOI: | 10.1143/jjap.36.l1075 |