此文章研究雷德保裝束(Rydberg-dressed)費米氣體在三維自由空間中的量子相轉變現象。由隨機相位近(random phase approximation)計算得知,若原子的雷德堡阻絕長度(Rydberg blockade length)夠長,或者系統密度夠高,微弱的交互作用即可使均勻的費米液體系統中出現有序密度波。我們的平均場理論(mean-field theory)結果顯示,系統經由一級相轉變過程形成具有體心立方晶格結構的有序密度波,並且其相轉變溫度約為費米能階的十分之一。再者,此研究涉及的理論徹底不同於已知的藍道費米液體理論,意即此有序密度結構非藍道費米液體理論所能預期。
We study quantum phase transitions of a repulsive Rydberg-dressed Fermi gas in 3D free space. Under random phase approximation(RPA), it is shown that a density wave order emerges from a Fermi liquid within week interaction and long blockade length (or high density) regime. Our mean-field theory results show that, this density wave order forms BCC structure through a first order phase transition, and the transition temperature is about one-tenth of the Fermi energy. Further- more, we argue that the theory associated with this novel phenomenon of repulsive Fermionic system differs completely from the well known Landau Fermi liquid theory.