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FERMI GAS WITH 4-FERMION BCS-TYPE INTERACTION

机译:费米气体与4费米恩BCS型相互作用

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A gas of spin 1/2 fermions with an interaction V + W = - ∑_(k,k′) g_(kk′)b_k~*b_(-k)~*b_(k′)b_(-k′), + ∑_k γkb_k~*b_k, where b_k = a_(k+)a_(k-) and a_(kσ), a_(k′σ′)~* satisfy Fermi anticommutation relations, is investigated. The trial ground state |G > is similar in form to the BCS ground state, with b_k~*b_(-k)~* replacing a_(k+)~*a_(-k-)~*, but because the excitation energies are not simply additive, the trial density matrix ρ_0 differs from the BCS one. The expectation values < G|H|G >and Tr(H ρ_0 ) are minimized, revealing the presence of a second-order phase transition, with T_c > T_(C(BCS)) for appropriately adjusted γ_k. It is shown that the minimization procedure applied leads to an expression tor the free energy density of H, which is asymptotically exact in the infinite-volume limit. Comparison with experimental data on high-temperature superconductors is made and for a particular choice of γ_k qualitative agreement is found with the temperature dependence of the order parameter of the BSCCO superconductor.
机译:具有相互作用V + W =-∑_(k,k')g_(kk')b_k〜* b _(-k)〜* b_(k')b _(-k')的自旋1/2费米子气体,+ ∑_kγkb_k〜* b_k,其中b_k = a_(k +)a_(k-)且a_(kσ),a_(k'σ')〜*满足费米反换向关系。试验基态| G>在形式上与BCS基态相似,但b_k〜* b _(-k)〜*代替了a_(k +)〜* a _(-k-)〜*,但是因为激发能是试验密度矩阵ρ_0与BCS有所不同,而不只是累加。期望值和Tr(Hρ_0)被最小化,表明存在二阶相变,对于适当调整的γ_k,T_c> T_(C(BCS))。结果表明,采用的最小化程序导致了H的自由能密度的表达式,它在无穷大极限内渐近精确。与高温超导体上的实验数据进行了比较,发现对于BSCCO超导体有序参数的温度依赖性,对γ_k定性选择的特定选择。

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