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弱异种相互作用双玻色混合物中两体关联的普适量子修正

Universal quantum corrections of two-body correlation in a weakly interspecies interacting binary Bose mixture

Rui-Yan Chen, Zhaoxin Liang, Gao Xianlong

arXiv 2608.17473首次发表:更新:

AI 中文总结

该研究采用Cornwall-Jackiw-Tomboulis两粒子不可约有效作用形式,推导弱耦合双玻色混合物两体关联的普适量子修正,重现Petrov物态方程并给出Lee-Huang-Yang外修正,分析质量失衡的影响。

AI 中文摘要

我们采用Cornwall-Jackiw-Tomboulis两粒子不可约有效作用形式,研究零温双玻色混合物中两体关联的普适量子修正。在弱异种耦合区域,基于Hubbard-Stratonovich变换的鞍点处理可结合双圈展开与无隙Hartree-Fock修正,从而保持Goldstone定理,并将耦合的双组分问题简化为两个可解析求解的单组分理论。在该框架内,我们推导了以气体参数低密展开形式呈现的基态能量密度,以及量子耗尽和化学势。结果显示其与单组分情况存在简单映射:通过将已知单组分级数在各组分的有效散射长度$a_{\rm{\tiny{\text{σ}\text{σ}}}}-a_{12}$处取值,可得到混合物的普适量子修正,其中$a_{\rm{\tiny{\text{σ}\text{σ}}}}$和$a_{12}$分别为组内和异种s波散射长度。这在弱耦合极限下于单圈阶重现了Petrov的物态方程,并在双圈阶给出了超出Lee-Huang-Yang的修正。我们还分析了质量失衡的作用,其通过精确重标因子$(1+m_1/m_2)/2$进入能量密度。

英文摘要

We investigate universal quantum corrections to two-body correlations in a zero-temperature binary Bose mixture using the Cornwall-Jackiw-Tomboulis two-particle-irreducible effective action formalism. In the weak interspecies-coupling regime, a saddle-point treatment based on Hubbard-Stratonovich transformations can be combined with a two-loop expansion and a gapless Hartree-Fock correction, thereby preserving the Goldstone theorem and reducing the coupled two-component problem to two analytically solvable single-component theories. Within this framework, we derive the ground-state energy density as a low-density expansion in the gas parameter, together with the quantum depletion and chemical potentials. The results exhibit a simple mapping to the single-component case: the universal quantum corrections of the mixture are obtained by evaluating the known single-component series at an effective scattering length $a_{σσ}-a_{12}$ for each species, where $a_{σσ}$ and $a_{12}$ are the intra- and interspecies $s$-wave scattering lengths. This reproduces Petrov's equation of state at one-loop order in the weak-coupling limit and yields beyond-Lee-Huang-Yang corrections at two-loop order. We also analyze the role of mass imbalance, which enters the energy density through the exact rescaling factor $(1+m_{1}/m_{2})/2$.

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