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Functional renormalization group for non-equilibrium quantum many-body problems  [PDF]
R. Gezzi,Th. Pruschke,V. Meden
Physics , 2006, DOI: 10.1103/PhysRevB.75.045324
Abstract: We extend the concept of the functional renormalization for quantum many-body problems to non-equilibrium situations. Using a suitable generating functional based on the Keldysh approach, we derive a system of coupled differential equations for the $m$-particle vertex functions. The approach is completely general and allows calculations for both stationary and time-dependent situations. As a specific example we study the stationary state transport through a quantum dot with local Coulomb correlations at finite bias voltage employing two different truncation schemes for the infinite hierarchy of equations arising in the functional renormalization group scheme.
Efimov physics from the functional renormalization group  [PDF]
Stefan Floerchinger,Sergej Moroz,Richard Schmidt
Physics , 2011, DOI: 10.1007/s00601-011-0231-z
Abstract: Few-body physics related to the Efimov effect is discussed using the functional renormalization group method. After a short review of renormalization in its modern formulation we apply this formalism to the description of scattering and bound states in few-body systems of identical bosons and distinguishable fermions with two and three components. The Efimov effect leads to a limit cycle in the renormalization group flow. Recently measured three-body loss rates in an ultracold Fermi gas $^6$Li atoms are explained within this framework. We also discuss briefly the relation to the many-body physics of the BCS-BEC crossover for two-component fermions and the formation of a trion phase for the case of three species.
Functional renormalization group approach to the BCS-BEC crossover  [PDF]
S. Diehl,S. Floerchinger,H. Gies,J. M. Pawlowski,C. Wetterich
Physics , 2009, DOI: 10.1002/andp.201010458
Abstract: The phase transition to superfluidity and the BCS-BEC crossover for an ultracold gas of fermionic atoms is discussed within a functional renormalization group approach. Non-perturbative flow equations, based on an exact renormalization group equation, describe the scale dependence of the flowing or average action. They interpolate continuously from the microphysics at atomic or molecular distance scales to the macroscopic physics at much larger length scales, as given by the interparticle distance, the correlation length, or the size of the experimental probe. We discuss the phase diagram as a function of the scattering length and the temperature and compute the gap, the correlation length and the scattering length for molecules. Close to the critical temperature, we find the expected universal behavior. Our approach allows for a description of the few-body physics (scattering and molecular binding) and the many-body physics within the same formalism.
Renormalization group, dimer-dimer scattering, and three-body forces  [PDF]
Boris Krippa,Niels R. Walet,Michael C. Birse
Physics , 2009, DOI: 10.1103/PhysRevA.81.043628
Abstract: We study the ratio between the fermion-fermion scattering length and the dimer-dimer scattering length for systems of nonrelativistic fermions, using the same functional renormalisation technique as previously applied to fermionic matter. We find a strong dependence on the cutoff function used in the renormalisation flow for a two-body truncation of the action. Adding a simple three-body term substantially reduces this dependence.
Summing parquet diagrams using the functional renormalization group: X-ray problem revisited  [PDF]
Philipp Lange,Casper Drukier,Anand Sharma,Peter Kopietz
Physics , 2015, DOI: 10.1088/1751-8113/48/39/395001
Abstract: We present a simple method for summing so-called parquet diagrams of fermionic many-body systems with competing instabilities using the functional renormalization group. Our method is based on partial bosonization of the interaction utilizing multi-channel Hubbard-Stratonovich transformations. A simple truncation of the resulting flow equations, retaining only the frequency-independent parts of the two-point and three-point vertices amounts to solving coupled Bethe-Salpeter equations for the effective interaction to leading logarithmic order. We apply our method by revisiting the X-ray problem and deriving the singular frequency dependence of the X-ray response function and the particle-particle susceptibility. Our method is quite general and should be useful in many-body problems involving strong fluctuations in several scattering channels.
Cluster Functional Renormalization Group  [PDF]
Johannes Reuther,Ronny Thomale
Physics , 2013, DOI: 10.1103/PhysRevB.89.024412
Abstract: Functional renormalization group (FRG) has become a diverse and powerful tool to derive effective low-energy scattering vertices of interacting many-body systems. Starting from a non-interacting expansion point of the action, the flow of the RG parameter Lambda allows to trace the evolution of the effective one-particle and two-particle vertices towards low energies by taking into account the vertex corrections between all parquet channels in an unbiased fashion. In this work, we generalize the expansion point at which the diagrammatic resummation procedure is initiated from a free UV limit to a cluster product state. We formulate a cluster FRG scheme where the non-interacting building blocks (i.e., decoupled spin clusters) are treated exactly, and the inter-cluster couplings are addressed via RG. As a benchmark study, we apply our cluster FRG scheme to the spin-1/2 bilayer Heisenberg model (BHM) on a square lattice where the neighboring sites in the two layers form the individual 2-site clusters. Comparing with existing numerical evidence for the BHM, we obtain reasonable findings for the spin susceptibility, magnon dispersion, and magnon quasiparticle weight even in coupling regimes close to antiferromagnetic order. The concept of cluster FRG promises applications to a large class of interacting electron systems.
Functional renormalization group approach to the four-body problem  [cached]
Schmidt R.,Moroz S.
EPJ Web of Conferences , 2010, DOI: 10.1051/epjconf/20100302006
Abstract: We present a renormalization group analysis of the non-relativistic four-boson problem by means of a simple model with pointlike three- and four-body interactions. We investigate in particular the unitarity point where the scattering length is in nite and all energies are at the atom threshold. We nd that the four-body problem behaves truly universally, independent of any four-body parameter con rming the ndings of Platter et al. and von Stecher et al. [1–3].
Three-body loss in lithium from functional renormalization  [PDF]
R. Schmidt,S. Floerchinger,C. Wetterich
Physics , 2008, DOI: 10.1103/PhysRevA.79.053633
Abstract: We use functional integral methods for an estimate of the three-body loss in a three-component $^6$Li ultracold atom gas. We advocate a simple picture where the loss proceeds by the formation of a three-atom bound state, the trion. In turn, the effective amplitude for the trion formation from three atoms is estimated from a simple effective boson exchange process. The energy gap of the trion and other key quantities for the loss coefficient are computed in a functional renormalization group framework.
Inverse problems in N-body scattering  [PDF]
Gunther Uhlmann,Andras Vasy
Mathematics , 2003,
Abstract: We survey finite energy inverse results in N-body scattering, and we also sketch the proof of the extension of our recent two-cluster to two-cluster three-body result to the many-body case: this requires only minor modifications. We also indicate how to extend a free-to-free inverse result in three-body scattering to the many-body case.
Functional renormalisation group for two-body scattering  [PDF]
Michael C. Birse
Physics , 2008, DOI: 10.1103/PhysRevC.77.047001
Abstract: The functional renormalisation group is applied to the effective action for scattering of two nonrelativistic fermions. The resulting physical effective action is shown to contain the correct threshold singularity. The corresponding "bare" action respects Galilean invariance up to second order in momenta. Beyond that order it contains terms that violate this symmetry and, for the particular regulator considered, nonanalytic third-order terms. The corresponding potential can be expanded around a nontrivial fixed point using the power counting appropriate to a system with large scattering length.
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