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arXiv 0901.0293cond-mat.mtrl-scicond-mat.supr-con
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无序存在下CaC6超导体的喇曼散射

Raman scattering from the CaC6 superconductor in the presence of disorder

A. Mialitsin, J. S. Kim, R. K. Kremer, G. Blumberg

摘要:

本文报道了CaC_6超导体的偏振喇曼散射。我们确定了两个三个拉曼活性Eg声子模式在440和1508 cm-1预期的R-3 m空间群的CaC 6。这些一阶散射模式与1300 cm-1和1600 cm-1附近的D和G带一起出现,它们的起源与普通石墨中的相应带相似。CaC 6中D和G带的强度与无序程度相关。D带由双共振拉曼散射过程产生;其频率作为激发能的函数以约35 cm-1/eV偏移。双共振喇曼散射探测有限波矢q的声子激发。我们估计的结构缺陷的特征间距约为100埃的规模通过比较的D带和1508 cm-1的Eg模式在CaC 6的校准强度比在无序石墨类似的频带。在Tc以下观察到一个24 cm-1的超导相干峰。

英文摘要:

Polarized Raman scattering has been performed on CaC6 superconductor. We identify two of the three Raman active Eg phonon modes at 440 and 1508 cm-1 expected for the R-3m space group of CaC6. These first order scattering modes appear along with the D and G bands around 1300 cm-1 and 1600 cm-1 that are similar in origin to the corresponding bands in plain graphite. The intensities of the D and G bands in CaC6 correlate with degree of disorder. The D band arises from the double resonant Raman scattering process; its frequency shifts as a function of excitation energy with approximately 35 cm-1/eV. The double resonant Raman scattering probes phonon excitations with finite wave vector q. We estimate the characteristic spacing of structural defects to be on the scale of about 100 Angstrom by comparing the intensity of the D band and the 1508 cm-1 Eg mode in CaC6 to calibrated intensity ratio of analogous bands in disordered graphites. A sharp superconducting coherence peak at 24 cm-1 is observed below Tc.

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