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Damping of zero sound in Luttinger liquids

机译:Luttinger液体中的零声音衰减

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摘要

We calculate the damping gamma(q) of collective density oscillations (zero sound) in a one-dimensional Fermi gas with dimensionless forward scattering interaction F and quadratic energy dispersion k(2)/2m at zero temperature. Using standard many-body perturbation theory, we obtain gamma(q) from the expansion of the inverse irreducible polarization to first order in the effective screened (RPA) interaction. For wave-vectors vertical bar q vertical bar/k(F) F (where k(F) = mv(F) is the Fermi wave-vector) we find to leading order gamma(q) proportional to vertical bar q vertical bar(3)/(v(F)m(2)). On the other hand, for F vertical bar q vertical bar/k(F) most of the spectral weight is carried by the particle-hole continuum, which is distributed over a frequency interval of the order of q(2)/m. We also show that zero sound damping leads to a finite maximum proportional to vertical bar k - k(F)vertical bar(-2+2 eta) of the charge peak in the single-particle spectral function, where eta is the anomalous dimension. Our prediction agrees with photoemission data for the blue bronze K0.3MoO3. We comment on other recent calculations of gamma(q).
机译:我们计算一维费米气体在零温度下具有无量纲的正向散射相互作用F和二次能量色散k(2)/ 2m的集体密度振荡(零声)的阻尼gamma(q)。使用标准的多体摄动理论,我们从不可逆反极化的展开到有效屏蔽(RPA)相互作用中的一阶,获得了gamma(q)。对于波矢量垂直条q垂直条/ k(F) F(其中k(F)= mv(F)是费米波矢量),我们发现与垂直条q垂直成比例的前导阶gamma(q) bar(3)/(v(F)m(2))。另一方面,对于F 竖线q竖线bar / k(F),大部分频谱权重由粒子-孔连续体承载,其分布在q(2)/ m量级的频率间隔上。我们还表明,零声音阻尼导致与单粒子光谱函数中电荷峰的竖线k-k(F)竖线k-k(F)竖线(-2 + 2 eta)成正比的有限最大值,其中eta是反常维度。我们的预测与蓝古铜K0.3MoO3的光发射数据一致。我们对gamma(q)的其他最新计算发表评论。

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