TY - JOUR
T1 - Magnetic ordering and quantum statistical effects in strongly repulsive Fermi-Fermi and Bose-Fermi mixtures
AU - Guan, X. W.
AU - Batchelor, M. T.
AU - Lee, J. Y.
PY - 2008/8/15
Y1 - 2008/8/15
N2 - We investigate magnetic properties and statistical effects in one-dimensional (1D) strongly repulsive two-component fermions and in a 1D mixture of strongly repulsive polarized fermions and bosons. Universality in the characteristics of phase transitions, magnetization, and susceptibility in the presence of an external magnetic field H are analyzed from the exact thermodynamic Bethe ansatz solution. We show explicitly that polarized fermions with a repulsive interaction have antiferromagnetic behavior at zero temperature. A universality class of linear field-dependent magnetization persists for weak and finite strong interaction. The system is fully polarized when the external field exceeds the critical value HcF ≈ 8 γ EF, where EF is the Fermi energy and γ is the dimensionless interaction strength. In contrast, the mixture of polarized fermions and bosons in an external field exhibits square-root field-dependent magnetization in the vicinities of H=0 and the critical value H= HcM ≈ 16 γ EF. We find that a pure boson phase occurs in the absence of the external field, fully polarized fermions and bosons coexist for 0<H< HcM, and a fully polarized fermion phase occurs for H≥ HcM. This phase diagram for the Bose-Fermi mixture is reminiscent of weakly attractive fermions with population imbalance, where the interacting fermions with opposite spins form singlet pairs.
AB - We investigate magnetic properties and statistical effects in one-dimensional (1D) strongly repulsive two-component fermions and in a 1D mixture of strongly repulsive polarized fermions and bosons. Universality in the characteristics of phase transitions, magnetization, and susceptibility in the presence of an external magnetic field H are analyzed from the exact thermodynamic Bethe ansatz solution. We show explicitly that polarized fermions with a repulsive interaction have antiferromagnetic behavior at zero temperature. A universality class of linear field-dependent magnetization persists for weak and finite strong interaction. The system is fully polarized when the external field exceeds the critical value HcF ≈ 8 γ EF, where EF is the Fermi energy and γ is the dimensionless interaction strength. In contrast, the mixture of polarized fermions and bosons in an external field exhibits square-root field-dependent magnetization in the vicinities of H=0 and the critical value H= HcM ≈ 16 γ EF. We find that a pure boson phase occurs in the absence of the external field, fully polarized fermions and bosons coexist for 0<H< HcM, and a fully polarized fermion phase occurs for H≥ HcM. This phase diagram for the Bose-Fermi mixture is reminiscent of weakly attractive fermions with population imbalance, where the interacting fermions with opposite spins form singlet pairs.
UR - http://www.scopus.com/inward/record.url?scp=49749128716&partnerID=8YFLogxK
U2 - 10.1103/PhysRevA.78.023621
DO - 10.1103/PhysRevA.78.023621
M3 - Article
SN - 1050-2947
VL - 78
JO - Physical Review A - Atomic, Molecular, and Optical Physics
JF - Physical Review A - Atomic, Molecular, and Optical Physics
IS - 2
M1 - 023621
ER -