2016
DOI: 10.1103/physreva.94.063650
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High-momentum distribution with a subleading k3 tail in odd-wave interacting one-dimensional Fermi gases

Abstract: We study the odd-wave interacting identical fermions in one-dimension with finite effective range. We show that to fully describe the high-momentum distribution ρ(k) up to k −4 , one needs four parameters characterizing the properties when two particles contact with each other. Two parameters are related to the variation of energy with respect to the odd-wave scattering length and the effective range, respectively, determining the k −2 tail and part of k −4 tail in ρ(k). The other two parameters are related to… Show more

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Cited by 33 publications
(30 citation statements)
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References 41 publications
(95 reference statements)
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“…Apart from this, there now appear several molecular states due to the different orientation of the angular momentum quantization of the molecule. As a result, the contact parameters has to be generalized which leads to a set of universal relations that has been discussed in detail in recent literature [16][17][18][19][20][21][22]. Explicit calculations of the p-wave contact within the Noziéres and Schmit-Rink formula has been carried out and finds general good agreement with the experimental findings [23].…”
Section: Introductionsupporting
confidence: 49%
“…Apart from this, there now appear several molecular states due to the different orientation of the angular momentum quantization of the molecule. As a result, the contact parameters has to be generalized which leads to a set of universal relations that has been discussed in detail in recent literature [16][17][18][19][20][21][22]. Explicit calculations of the p-wave contact within the Noziéres and Schmit-Rink formula has been carried out and finds general good agreement with the experimental findings [23].…”
Section: Introductionsupporting
confidence: 49%
“…formally as Eqs. (26) and (27). Analogously, by subtracting [27] * × Ψ from Ψ ′ * × [26], and integrating over the domain D ǫ , the set of all configurations (r i , r j ) in which r = |r i − r j | > ǫ, we obtain…”
Section: A Adiabatic Energy Relationsmentioning
confidence: 99%
“…All these relations are characterized by the only universal quantity named contact, and therefore known as the contact theory. During past few years, the concept of contact theory was further generalized to higher-partial-wave interactions [13][14][15][16][17][18][19][20] as well as to low dimensions [21][22][23][24][25][26][27][28][29], and more contacts appear when additional two-body parameters are involved.…”
Section: Introductionmentioning
confidence: 99%
“…One can relate the bare parameters of the odd-wave interaction (λ and ν) to the physical scattering parameters by calculating diagrammatically the two-body scattering amplitude [33]:…”
Section: B Odd-wave Interactionmentioning
confidence: 99%
“…(19), we arrive to the total Lagrangian L = L σ + L (0) ρ + L ρσ given by Eqs. (31) - (33) in the main text. The coefficients in the Lagrangian are given by…”
Section: Total Bosonized Lagrangianmentioning
confidence: 99%