scholarly journals Pair Correlations of a Spin-Imbalanced Fermi Gas on Two-Leg Ladders

2009 ◽  
Vol 102 (7) ◽  
Author(s):  
A. E. Feiguin ◽  
F. Heidrich-Meisner
Keyword(s):  
2008 ◽  
Vol 78 (5) ◽  
Author(s):  
S. Riedl ◽  
E. R. Sánchez Guajardo ◽  
C. Kohstall ◽  
A. Altmeyer ◽  
M. J. Wright ◽  
...  

2010 ◽  
Vol 105 (7) ◽  
Author(s):  
E. D. Kuhnle ◽  
H. Hu ◽  
X.-J. Liu ◽  
P. Dyke ◽  
M. Mark ◽  
...  

2013 ◽  
Vol 111 (26) ◽  
Author(s):  
Vudtiwat Ngampruetikorn ◽  
Jesper Levinsen ◽  
Meera M. Parish

2020 ◽  
Vol 22 (8) ◽  
pp. 083008
Author(s):  
M Pini ◽  
P Pieri ◽  
M Jäger ◽  
J Hecker Denschlag ◽  
G Calvanese Strinati

2010 ◽  
Vol 108 (1) ◽  
pp. 51-54 ◽  
Author(s):  
Soon-Yong Chang ◽  
Mohit Randeria ◽  
Nandini Trivedi

We address the question of ferromagnetism in repulsive Fermi gas, a problem of fundamental interest, using quantum Monte Carlo simulations that include backflow corrections. We investigate a two-component Fermi gas on the upper branch of a Feshbach resonance and contrast it with the hard-sphere gas. We find that, in both cases, the Fermi liquid becomes unstable to ferromagnetism at a kFa smaller than the mean field result, where kF is the Fermi wavevector and a is the scattering length. Even though the total energies E(kFa) are similar in the two cases, their pair correlations and kinetic energies are completely different, reflecting the underlying potentials. We discuss the extent to which our calculations shed light on recent experiments.


2006 ◽  
Vol 97 (10) ◽  
Author(s):  
C. Lobo ◽  
I. Carusotto ◽  
S. Giorgini ◽  
A. Recati ◽  
S. Stringari

2015 ◽  
Vol 11 (3) ◽  
pp. 3224-3228
Author(s):  
Tarek El-Ashram

In this paper we derived a new condition of formation and stability of all crystalline systems and we checked its validity andit is found to be in a good agreement with experimental data. This condition is derived directly from the quantum conditionson the free electron Fermi gas inside the crystal. The new condition relates both the volume of Fermi sphere VF andvolume of Brillouin zone VB by the valence electron concentration VEC as ;𝑽𝑭𝑽𝑩= 𝒏𝑽𝑬𝑪𝟐for all crystalline systems (wheren is the number of atoms per lattice point).


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