scholarly journals Light scattering study of low-energy vibrational excitations in the metallic glass Ni67Zr33using electronic Raman scattering

2011 ◽  
Vol 84 (10) ◽  
Author(s):  
B. Muschler ◽  
I. Tüttő ◽  
A. Zawadowski ◽  
J. Balogh ◽  
R. Hackl
1997 ◽  
Vol 56 (18) ◽  
pp. R11427-R11430 ◽  
Author(s):  
Moonsoo Kang ◽  
G. Blumberg ◽  
M. V. Klein ◽  
N. N. Kolesnikov

1992 ◽  
Vol 81 (5) ◽  
pp. 407-410 ◽  
Author(s):  
A.A. Maksimov ◽  
A.V. Puchkov ◽  
I.I. Tartakovskii ◽  
V.B. Timofeev ◽  
D. Reznik ◽  
...  

1986 ◽  
Vol 34 (9) ◽  
pp. 6235-6239 ◽  
Author(s):  
S. L. Cooper ◽  
M. V. Klein ◽  
Z. Fisk ◽  
J. L. Smith

1994 ◽  
Vol 50 (1) ◽  
pp. 150-157 ◽  
Author(s):  
G. S. Nolas ◽  
V. G. Tsoukala ◽  
S. K. Gayen ◽  
Glen A. Slack

1991 ◽  
Vol 43 (4) ◽  
pp. 3752-3755 ◽  
Author(s):  
D. Kirillov ◽  
C. B. Eom ◽  
T. H. Geballe

1985 ◽  
Vol 31 (3) ◽  
pp. 1490-1497 ◽  
Author(s):  
S. Venugopalan ◽  
Mitra Dutta ◽  
A. K. Ramdas ◽  
J. P. Remeika

1992 ◽  
Vol 06 (23n24) ◽  
pp. 4019-4024 ◽  
Author(s):  
V.N. Denisov ◽  
A.A. Zakhidov ◽  
R. Danieli ◽  
G. Ruani ◽  
R. Zamboni ◽  
...  

The Raman scattering study of superconducting thin films of A 3 C 60 (A=K,Rb) carried out upon laser excitations at 1.16 and 2.41 eV have revealed the significant broadening and Fano-lineshapes of several low energy H g intramolecular modes with relative intensities and widths depending on excitation energies. The most interesting feature of the 1.16 eV excited spectrum is the wide asymmetric band at 400 cm −1 which can be assigned by Fano-shape fitting to enormously broadened H g (2) mode red shifted compared to its bare frequency of 408 cm −1. The narrowing of all lower H g modes in insulating A 6 C 60 phase indicates strong electron-phonon coupling of this Jahn-Teller modes in x =3 phase and suggests that this low energy vibrations are contributing to superconducting pairing. However the possibility to interpret the wide band at 400 cm −1 as the maximum of electronic background can not be ruled out yet and is supported by our preliminary observations of its disappearance at low temperature below T c .


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