Department of Physics, University of California, Berkeley, California 94720, USA.
Phys Rev Lett. 2012 Dec 7;109(23):237004. doi: 10.1103/PhysRevLett.109.237004. Epub 2012 Dec 5.
We study the structure of Bogoliubov quasiparticles, bogolons, the fermionic excitations of paired superfluids that arise from fermion (BCS) pairing, including neutral superfluids, superconductors, and paired quantum Hall states. The naive construction of a stationary quasiparticle in which the deformation of the pair field is neglected leads to a contradiction: it carries a net electrical current even though it does not move. However, treating the pair field self-consistently resolves this problem: in a neutral superfluid, a dipolar current pattern is associated with the quasiparticle for which the total current vanishes. When Maxwell electrodynamics is included, as appropriate to a superconductor, this pattern is confined over a penetration depth. For paired quantum Hall states of composite fermions, the Maxwell term is replaced by a Chern-Simons term, which leads to a dipolar charge distribution and consequently to a dipolar current pattern.
我们研究了玻戈留波夫准粒子(bogolon)的结构,玻戈留波夫准粒子是由费米子(BCS 配对)配对产生的配对超流体的费米子激发,包括中性超流体、超导体和配对量子霍尔态。在一个静止的准粒子的简单构造中,忽略了对配对场的变形,这导致了一个矛盾:它携带净电流,尽管它没有移动。然而,通过自洽地处理配对场,可以解决这个问题:在中性超流体中,与准粒子相关联的是偶极电流模式,其中总电流为零。当包括麦克斯韦电磁学时,这适用于超导体,这种模式被限制在穿透深度内。对于复合费米子的配对量子霍尔态,麦克斯韦项被一个陈-西蒙斯项所取代,这导致了偶极电荷分布,进而导致了偶极电流模式。