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基于Balseiro和Falicov的概念,我们用一个简单模型计算了电荷密度波(CDW)与超导共存系统中被电声子相互作用重整化的CDW振幅模式的谱函数A(ω),所得的A(ω)在ω≤2G(G为CDW带隙)区域有一个权重相当大的δ函数型的峰,而在ω>2(G2十△2)1/2(△为超导能隙)区域是比较宽的连续谱,固定G,当△减少时峰的强度显著降低,但其位置仅有较小的变化;与此同时连续谱的权重增加,这些特点与Sooryakumar和Klein在电荷密度波超导体2H-Nbse2中发现的喇曼出线的能隙模式的行为是一致的。Following the idea put forward by Balseiro and Falicov, we have calculated the renor-malized spectral function A (ω) of the amplitude mode of Charge-Density-wave (CDW) phonon by electron-phonon interaction in a model system with coexisting CDW and superconductivity. The A(ω) obtained shows a havily weighted peak of delta-function type at the frequency ω≤2G, where G is the CDW band gap, and a relatively broad continuous spectrum in the region ω>2(G2十△2)1/2, where △ is the superconducting energy gap. Under the condition of fixed G, as △ decreases the intensity of the peak decreases considerably with only a small shift in its position, while the weight of the continuous spectrum raises. These characteristics are in agreement with the behavior of the Raman-active gap modes found by Sooryakumar and Klein in CDW superconductor 2H-NbSe2.
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