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PhD thesis in English

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4. Mean-field description of an <strong>in</strong>teract<strong>in</strong>g BECconta<strong>in</strong>s terms up to the 4 th order <strong>in</strong> δψ that we should <strong>in</strong>tegrate over. Withoutfurther approximations, however, this problem is equivalent to the orig<strong>in</strong>al functional<strong>in</strong>tegral. Numerous approximation techniques were developed to treat terms of the3 rd and 4 th order <strong>in</strong> different approximative ways [19, 82]. In the Hartree-Fock-Bogoliubov approach, we approximate the 4 th order term asδψ ∗ δψ δψ ∗ δψ ≈4〈δψ ∗ δψ〉δψ ∗ δψ + 〈δψ ∗ δψ ∗ 〉δψδψ + 〈δψδψ〉δψ ∗ δψ ∗−2〈δψ ∗ δψ〉〈δψ ∗ δψ〉 − 〈δψδψ〉〈δψ ∗ δψ ∗ 〉. (4.7)In accordance with the previous decomposition, we <strong>in</strong>troduce auxiliary functionsh(⃗r, τ;⃗r, τ) = 〈δψ ∗ (⃗r, τ)δψ(⃗r, τ)〉 ,f(⃗r, τ;⃗r ′ , τ ′ ) = 〈δψ ∗ (⃗r, τ)δψ(⃗r ′ , τ ′ )〉 ,b(⃗r, τ;⃗r ′ , τ ′ ) = 〈δψ(⃗r, τ)δψ(⃗r ′ , τ ′ )〉 ,which are denoted as Hartree, Fock and Bogoliubov term, respectively. At themoment, the <strong>in</strong>troduced average values are purely formal, but can be later def<strong>in</strong>edso as to make the complete procedure self-consistent. In the case of the contact<strong>in</strong>teraction (1.21), the Hartree and Fock terms yield equal contributions, hence afactor of 4 <strong>in</strong> front of the correspond<strong>in</strong>g term <strong>in</strong> Eq. (4.7).After apply<strong>in</strong>g the mean-field approximation (4.7), the action A E becomes quadratic<strong>in</strong> δψ, and now the functional <strong>in</strong>tegrations of the Gaussian <strong>in</strong>tegrals can be explicitlyperformed. The f<strong>in</strong>al result for the partition function can be written <strong>in</strong> theformZ(β) = e −β Γ eff[ψ,ψ ∗ ,h,f,b] , (4.8)where Γ eff is the effective action, def<strong>in</strong>ed as a functional of five arguments: ψ(⃗r, τ),ψ ∗ (⃗r, τ), h(⃗r, τ;⃗r, τ), f(⃗r, τ;⃗r ′ , τ ′ ) and b(⃗r, τ;⃗r ′ , τ ′ ). They are determ<strong>in</strong>ed by extremiz<strong>in</strong>gthe effective action Γ eff [ψ, ψ ∗ , h, f, b] with respect to each of them:δΓ effδψ = 0, δΓ effδψ ∗= 0, δΓ effδh = 0, δΓ effδf = 0, δΓ effδb= 0.In the quest for the simplest mean-field description of an <strong>in</strong>homogeneous BEC,we will make another simplification by neglect<strong>in</strong>g Bogoliubov terms, i.e. anomalouscorrelations b(⃗r, τ;⃗r ′ , τ ′ ), as discussed <strong>in</strong> Ref. [83]. This assumption is justified <strong>in</strong>86

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