Electronic Raman scattering in optimally doped Tl-2201

L. V. Gasparov; P. Lemmens; M. Brinkmann; N. Kolesnikov; G. Güntherodt

doi:10.1007/BF02583859

Electronic Raman scattering in optimally doped Tl-2201

L. V. Gasparov
, P. Lemmens
, M. Brinkmann
, N. Kolesnikov
, G. Güntherodt

Producción científica: Article › revisión exhaustiva

Resumen

We present polarized Raman spectra of nearly optimally doped single crystals of Tl2Ba2CuO6 (Tc=80K and 90K). The peak positions in the B1g component of the electronic Raman scattering are found at 460cm−1 (T c =90K), or 430cm−1 (T c =80K) which corresponds to 2Δ max /κ B T C =7.6 ± 0.4. The A1g - and B2g -symmetry components show smaller values for the peak positions and decrease linearly inw toward lower frequencies while the B1g scattering component shows a decrease cubic inw. The temperature dependence of the B1g scattering component reveals a deviation from BCS behavior. Experimental data are explained on the basis of a dx 2−y2-wave symmetry of the order parameter.

Idioma original	American English
Publicación	Czechoslovak Journal of Physics
Volumen	46
DOI	https://doi.org/10.1007/BF02583859
Estado	Published - feb 1 1996
Publicado de forma externa	Sí

Disciplines

Atomic, Molecular and Optical Physics
Physics
Quantum Physics

Acceder al documento

10.1007/BF02583859Licencia: Unspecified

Otros archivos y enlaces

Link to publication

Citar esto

@article{e169d95a30204596bfd3a4fcaa4ee30b,

title = "Electronic Raman scattering in optimally doped Tl-2201",

abstract = "We present polarized Raman spectra of nearly optimally doped single crystals of Tl2Ba2CuO6 (Tc=80K and 90K). The peak positions in the B1g component of the electronic Raman scattering are found at 460cm−1 (T c =90K), or 430cm−1 (T c =80K) which corresponds to 2Δ max /κ B T C =7.6 ± 0.4. The A1g - and B2g -symmetry components show smaller values for the peak positions and decrease linearly inw toward lower frequencies while the B1g scattering component shows a decrease cubic inw. The temperature dependence of the B1g scattering component reveals a deviation from BCS behavior. Experimental data are explained on the basis of a dx 2−y2-wave symmetry of the order parameter.",

author = "Gasparov, \{L. V.\} and P. Lemmens and M. Brinkmann and N. Kolesnikov and G. G{\"u}ntherodt",

note = "We present polarized Raman spectra of nearly optimally doped single crystals of Tl2Ba2CuO6 (Tc=80K and 90K). The peak positions in the B1g component of the electronic Raman scattering are found at 460",

year = "1996",

month = feb,

day = "1",

doi = "10.1007/BF02583859",

language = "American English",

volume = "46",

journal = "Czechoslovak Journal of Physics",

issn = "0011-4626",

}

TY - JOUR

T1 - Electronic Raman scattering in optimally doped Tl-2201

AU - Gasparov, L. V.

AU - Lemmens, P.

AU - Brinkmann, M.

AU - Kolesnikov, N.

AU - Güntherodt, G.

N1 - We present polarized Raman spectra of nearly optimally doped single crystals of Tl2Ba2CuO6 (Tc=80K and 90K). The peak positions in the B1g component of the electronic Raman scattering are found at 460

PY - 1996/2/1

Y1 - 1996/2/1

N2 - We present polarized Raman spectra of nearly optimally doped single crystals of Tl2Ba2CuO6 (Tc=80K and 90K). The peak positions in the B1g component of the electronic Raman scattering are found at 460cm−1 (T c =90K), or 430cm−1 (T c =80K) which corresponds to 2Δ max /κ B T C =7.6 ± 0.4. The A1g - and B2g -symmetry components show smaller values for the peak positions and decrease linearly inw toward lower frequencies while the B1g scattering component shows a decrease cubic inw. The temperature dependence of the B1g scattering component reveals a deviation from BCS behavior. Experimental data are explained on the basis of a dx 2−y2-wave symmetry of the order parameter.

AB - We present polarized Raman spectra of nearly optimally doped single crystals of Tl2Ba2CuO6 (Tc=80K and 90K). The peak positions in the B1g component of the electronic Raman scattering are found at 460cm−1 (T c =90K), or 430cm−1 (T c =80K) which corresponds to 2Δ max /κ B T C =7.6 ± 0.4. The A1g - and B2g -symmetry components show smaller values for the peak positions and decrease linearly inw toward lower frequencies while the B1g scattering component shows a decrease cubic inw. The temperature dependence of the B1g scattering component reveals a deviation from BCS behavior. Experimental data are explained on the basis of a dx 2−y2-wave symmetry of the order parameter.

UR - https://link.springer.com/article/10.1007/BF02583859

U2 - 10.1007/BF02583859

DO - 10.1007/BF02583859

M3 - Article

SN - 0011-4626

VL - 46

JO - Czechoslovak Journal of Physics

JF - Czechoslovak Journal of Physics

ER -