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arXiv:1211.6679 · Physical Review A

Dimer-dimer scattering length for fermions with different masses: Analytical study for large mass ratio

Florent Alzetto, R. Combescot, X. Leyronas

Published Feb 7, 2013• 13 citations
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Abstract

We study the dimer-dimer scattering length ${a}_{4}$ for a two-component Fermi mixture in which the different fermions have different masses ${m}_{\ensuremath{\uparrow}}$ and ${m}_{\ensuremath{\downarrow}}$. This is made in the framework of the exact field-theoretic method. In the large mass ratio domain the equations are simplified enough to lead to an analytical solution. In particular we link ${a}_{4}$ to the fermion-dimer scattering length ${a}_{3}$ for the same fermions and obtain the very simple relation ${a}_{4}={a}_{3}/2$. The result ${a}_{4}\ensuremath{\simeq}{a}_{3}/2$ is actually valid whatever the mass ratio with quite good precision. As a result we find an analytical expression providing ${a}_{4}$ with fairly good precision for any mass. To dominant orders for large mass ratio it agrees with the literature. We show that in this large mass ratio domain, the dominant processes are the repeated dimer-dimer Born scatterings, considered earlier by Pieri and Strinati [Phys Rev. B 61, 15370 (2000)]. We conclude that their approximation of retaining only these processes is a fairly good one whatever the mass ratio.

DOI
10.1103/physreva.87.022704

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We study the dimer-dimer scattering length a4{a}_{4}a4​ for a two-component Fermi mixture in which the different fermions have different masses m\ensuremath↑{m}_{\ensuremath{\uparrow}}m\ensuremath↑​ and m\ensuremath↓{m}_{\ensuremath{\downarrow}}m\ensuremath↓​. This is made in the framework of the exact field-theoretic method. In the large mass ratio domain the equations are simplified enough to lead to an analytical solution. In particular we link a4{a}_{4}a4​ to the fermion-dimer scattering length a3{a}_{3}a3​ for the same fermions and obtain the very simple relation a4=a3/2{a}_{4}={a}_{3}/2a4​=a3​/2. The result a4\ensuremath≃a3/2{a}_{4}\ensuremath{\simeq}{a}_{3}/2a4​\ensuremath≃a3​/2 is actually valid whatever the mass ratio with quite good precision. As a result we find an analytical expression providing a4{a}_{4}a4​ with fairly good precision for any mass. To dominant orders for large mass ratio it agrees with the literature. We show that in this large mass ratio domain, the dominant processes are the repeated dimer-dimer Born scatterings, considered earlier by Pieri and Strinati [Phys Rev. B 61, 15370 (2000)]. We conclude that their approximation of retaining only these processes is a fairly good one whatever the mass ratio.
We consider the problem of obtaining the scattering length for a fermion colliding with a dimer, formed from a fermion identical to the incident one and another different fermion. This is done in the universal regime where the range of interactions is short enough that the scattering length aaa for nonidentical fermions is the only relevant quantity. This is the generalization to fermions with different masses of the problem solved long ago by Skorniakov and Ter-Martirosian for particles with equal masses. We solve this problem analytically in the two limiting cases where the mass of the solitary fermion is very large or very small compared to the mass of the two other identical fermions. This is done for both the value of the scattering length and the function entering the Skorniakov--Ter-Martirosian integral equation, for which simple explicit expressions are obtained.
We consider systems of two-component fermions with unequal masses and interacting via a short-range attractive potential. We discuss the case where the two-component fermions form a shallow dimer with large scattering length. The three-fermion and four-fermion systems with such properties are universal and characterized by the twofermion scattering length aff and the ratio of the mass of spin-↑ fermion to the mass of spin-↓ fermion, m↑/m↓. In this study, using lattice effective field theory, we analyze fermion-dimer and dimer-dimer systems and calculate the universal fermion-dimer and dimer-dimer scattering lengths for various values of the mass ratio m↑/m↓. We find that these universal scattering lengths increase logarithmically with the mass ratio m↑/m↓.
We use the diagrammatic TTT-matrix approach to analyze the three-body scattering problem between two identical fermions and a third particle (which could be a different species of fermion or a boson). We calculate the sss-wave dimer-atom scattering length for all mass ratios, and our results exactly match the results of Petrov. In particular, we list the exact dimer-atom scattering lengths for all available two-species Fermi-Fermi and Bose-Fermi mixtures. In addition, unlike that of the equal-mass-particles case where the three-body scattering TTT matrix decays monotonically as a function of the outgoing momentum, we show that, after an initial rapid drop, this function changes sign and becomes negative at large momenta and then decays slowly to zero when the mass ratio of the fermions to the third particle is higher than a critical value (around 6.56.56.5). As the mass ratio gets higher, modulations of the TTT matrix become more apparent with multiple sign changes, related to the ``fall of a particle to the center'' phenomenon and to the emergence of three-body Efimov bound states.
We study near a Feshbach resonance, as a function of the mass ratio, the fermion-dimer scattering amplitude in fermionic mixtures of two fermion species. When masses are equal the physical situation is known to be quite simple. We show that, when the mass ratio is increased, the situation becomes much more complex. For the sss-wave contribution we obtain an analytical solution in the asymptotic limit of very large mass ratio. In this regime the sss-wave scattering amplitude displays a large number of zeros, essentially linked to the known large value of the fermion-dimer scattering length in this regime. We find by an exact numerical calculation that a zero is still present for a mass ratio of 15. For the ppp-wave contribution we make our study below the mass ratio of 8.17, where a fermion-dimer bound state appears. We find that a strong ppp-wave resonance is present at low energy, due to a virtual bound state, in the fermion-dimer system, which is a forerunner of the real bound state. This resonance becomes prominent in the mass ratio range around the one corresponding to the 40{}^{40}40K -6{}^{6}6Li mixtures, much studied experimentally. This resonance should affect a number of physical properties. These include the equation of state of unbalanced mixtures at very low temperature but also the equation of state of balanced mixtures at moderate or high temperature. The frequency and the damping of collective modes should also provide a convenient way to evidence this resonance. Finally it should be possible to modify the effective mass of one of the fermionic species by making use of an optical lattice. This would allow one to study the strong dependence of the resonance as a function of the mass ratio of the two fermionic elements. In particular one could check if the virtual bound state is relevant for the instabilities of these mixtures.
Mixtures of polarized fermions of two different masses can form weakly bound clusters, such as dimers and trimers, that are universally described by the scattering length between the heavy and light fermions.We use the resonating group method to investigate the low-energy scattering processes involving dimers or trimers.The method reproduces approximately the known particle-dimer and dimer-dimer scattering lengths.We use it to estimate the trimer-trimer scattering length, which is presently unknown, and find it to be positive.
Using the diagrammatic approach, here we study how spin-orbit coupling (SOC) affects the fermion-dimer and dimer-dimer scattering lengths in the Born approximation, and we benchmark their accuracy with the higher-order approximations. We consider both isotropic and Rashba couplings in three dimensions and show that the Born approximation gives accurate results in the $1/(m\ensuremath{\alpha}{a}_{s})\ensuremath{\ll}\ensuremath{-}1$ limit, where mmm is the mass of the fermions, $\ensuremath{\alpha}$ is the strength of the SOC, and as{a}_{s}as​ is the sss-wave scattering length between fermions. This is because the higher-loop contributions form a perturbative series in the $1/(m\ensuremath{\alpha}{a}_{s})<0$ region that is controlled by the smallness of the residue ZZZ of the dimer propagator. In sharp contrast, since ZZZ grows with the square root of the binding energy of the dimer in the $1/(m\ensuremath{\alpha}{a}_{s})>0$ region, all of the higher-loop contributions are of similar order.