Department of Physics, The University of Texas at Dallas, Richardson, Texas 75080, USA.
Phys Rev Lett. 2012 Sep 7;109(10):105302. doi: 10.1103/PhysRevLett.109.105302. Epub 2012 Sep 5.
Recent experimental breakthroughs in realizing spin-orbit (SO) coupling for cold atoms have spurred considerable interest in the physics of two-dimensional SO coupled Fermi superfluids, especially topological Majorana fermions (MFs) which were predicted to exist at zero temperature. However, it is well known that long-range superfluid order is destroyed in two dimensions by phase fluctuations at finite temperature, and the relevant physics is the BKTs transition. In this Letter, we examine finite temperature effects on SO coupled Fermi gases and show that finite temperature is indeed necessary for the observation of MFs. Majorana fermions are topologically protected by a quasiparticle energy gap which is found to be much larger than the temperature. The restrictions to the parameter region for the observation of MFs have been obtained.
最近在实现冷原子自旋轨道(SO)耦合方面的实验突破,激发了人们对二维 SO 耦合费米超流体物理的极大兴趣,特别是在零温度下预测存在的拓扑马约拉纳费米子(MFs)。然而,众所周知,在有限温度下,二维的长程超流序会被相位涨落破坏,相关物理是 BKT 相变。在这封信中,我们研究了 SO 耦合费米气体的有限温度效应,并表明有限温度对于观察 MF 是非常必要的。MFs 由准粒子能隙拓扑保护,发现该能隙远大于温度。已经获得了观察 MF 的参数区域的限制。