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arXiv 2410.13596gr-qccond-mat.quant-gas

玻色-爱因斯坦凝聚体数量守恒类比引力中的量子非线性效应

Quantum nonlinear effects in the number-conserving analogue gravity of Bose-Einstein condensates

Kunal Pal, Uwe R. Fischer

AI总结:

本文研究了绝对零度下玻色-爱因斯坦凝聚体的量子动力学,提出超越 Unruh 线性化范式的非线性类比引力模型,通过引入量子涨落重整化时空度规、矢量场和质量项来考虑准粒子反作用,并应用于宇宙学度规。

摘要:

我们研究了绝对零度下玻色-爱因斯坦凝聚体的量子动力学,并证明超越 Unruh 标准线性化类比引力范式的类比引力模型必须考虑准粒子激发对凝聚体背景的反作用。这要求将微扰幅度展开至二阶,从而考虑理论的内禀非线性。结果表明,标准范式发生了重大修正。具体而言,为了获得二阶微扰在弯曲时空中完全 Lorentz 协变的方程,我们证明有必要在形式平均场展开参数 $N^{-1/2}$(其中 $N$ 为总粒子数)的幂次中引入主导阶的量子涨落重整化时空度规,该度规与 Unruh 声学时空度规显著不同,并在次主导阶 $1/N$ 引入两个涌现矢量场和一个质量项。重整化度规、矢量场和质量项均记录了准粒子对凝聚体的反作用,精度达到所考虑的 $N^{-1/2}$ 幂次阶。最后,我们将该形式体系应用于类比宇宙学的 Friedmann-Lemaître-Robertson-Walker 度规,并确立了由激发云施加的量子多体反作用导致的重整化形式。

英文摘要:

We consider the quantum dynamics of Bose-Einstein condensates at absolute zero, and demonstrate that an analogue gravity model going beyond the standard linearized analogue gravity paradigm à la Unruh must take into account the backreaction of quasiparticle excitations onto the condensate background. This requires that one expands to second order in perturbation amplitude and thus takes the intrinsic nonlinearity of the theory into account. It is shown that, as a result, significant modifications of the standard paradigm occur. In particular, to obtain a fully Lorentz-covariant equation in curved spacetime for second-order perturbations, we demonstrate that it is necessary to introduce, to leading order in powers of the formal mean-field expansion parameter $N^{-1/2}$ (where $N$ is total particle number), a quantum-fluctuation-renormalized spacetime metric which substantially differs from the Unruh acoustic spacetime metric and, to subleading order $1/N$, two emergent vector fields and a mass term. Both the renormalized metric as well as the vector fields and the mass then keep track of the backreaction of the quasiparticles onto the condensate up to the order in powers of $N^{-1/2}$ considered. Finally, we apply our formalism to an analogue-cosmological Friedmann-Lemaître-Robertson-Walker metric and establish its renormalized form due to the quantum many-body backreaction exerted by the excitation cloud.

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