We consider the thermodynamics of a homogeneous superfluid dilute Bose gas in the presence of weak quenched disorder. Following the zero-temperature approach of Huang and Meng, we diagonalize the Hamiltonian of a dilute Bose gas in an external random delta-correlated potential by means of a Bogoliubov transformation. We extend this approach to finite temperature by combining the Popov and the many-body T-matrix approximations. This approach permits us to include the quasiparticle interactions within this temperature range. We derive the disorder-induced shifts of the Bose-Einstein critical temperature and of the temperature for the onset of superfluidity by approaching the transition points from below, i.e., from the superfluid phase. Our results lead to a phase diagram consistent with that of the finite-temperature theory of Lopatin and Vinokur which was based on the replica method, and in which the transition points were approached from above.
%0 Journal Article
%1 falco2007
%A Falco, G. M.
%A Pelster, A.
%A Graham, R.
%D 2007
%J Physical Review A
%K GAS
%N 6
%P 063619
%R 10.1103/PhysRevA.75.063619
%T Thermodynamics of a Bose-Einstein condensate with weak disorder
%V 75
%X We consider the thermodynamics of a homogeneous superfluid dilute Bose gas in the presence of weak quenched disorder. Following the zero-temperature approach of Huang and Meng, we diagonalize the Hamiltonian of a dilute Bose gas in an external random delta-correlated potential by means of a Bogoliubov transformation. We extend this approach to finite temperature by combining the Popov and the many-body T-matrix approximations. This approach permits us to include the quasiparticle interactions within this temperature range. We derive the disorder-induced shifts of the Bose-Einstein critical temperature and of the temperature for the onset of superfluidity by approaching the transition points from below, i.e., from the superfluid phase. Our results lead to a phase diagram consistent with that of the finite-temperature theory of Lopatin and Vinokur which was based on the replica method, and in which the transition points were approached from above.
@article{falco2007,
abstract = {We consider the thermodynamics of a homogeneous superfluid dilute Bose gas in the presence of weak quenched disorder. Following the zero-temperature approach of Huang and Meng, we diagonalize the Hamiltonian of a dilute Bose gas in an external random delta-correlated potential by means of a Bogoliubov transformation. We extend this approach to finite temperature by combining the Popov and the many-body T-matrix approximations. This approach permits us to include the quasiparticle interactions within this temperature range. We derive the disorder-induced shifts of the Bose-Einstein critical temperature and of the temperature for the onset of superfluidity by approaching the transition points from below, i.e., from the superfluid phase. Our results lead to a phase diagram consistent with that of the finite-temperature theory of Lopatin and Vinokur which was based on the replica method, and in which the transition points were approached from above.},
added-at = {2012-12-07T18:53:37.000+0100},
af = {Falco, G. M.EOLEOLPelster, A.EOLEOLGraham, R.},
author = {Falco, G. M. and Pelster, A. and Graham, R.},
biburl = {https://www.bibsonomy.org/bibtex/24147d421f0fe1ca83c54a164c78750f9/jabreftest},
citedreferences = {Andersen JO, 2002, PHYS REV LETT, V88, DOI 10.1103/PhysRevLett.88.070407 ; Astrakharchik GE, 2002, PHYS REV A, V66, DOI 10.1103/PhysRevA.66.0236XX ; ATKINS KR, 1959, PHYS REV, V113, P962, DOI 10.1103/PhysRev.113.962 ; BELIAEV ST, 1958, SOV PHYS JETP-USSR, V7, P289 ; Beliaev S. T., 1958, SOV PHYS JETP, V7, P104 ; Bijlsma M, 1997, PHYS REV A, V55, P498, DOI 10.1103/PhysRevA.55.498 ; Bogolurov N.F., 1947, Journal of Physics, V11 ; FALCO GM, UNPUB PHYS REV A ; FISHER DS, 1988, PHYS REV B, V37, P4936, DOI 10.1103/PhysRevB.37.4936 ; GIORGINI S, 1994, PHYS REV B, V49, P12938, DOI 10.1103/PhysRevB.49.12938 ; GRAHAM R, CONDMAT0508306 ; HUANG K, 1992, PHYS REV LETT, V69, P644, DOI 10.1103/PhysRevLett.69.644 ; HUANG K, 1957, PHYS REV, V105, P767, DOI 10.1103/PhysRev.105.767 ; KHALATNIKOV IM, 1965, INTRO THEORY SUPERFL ; Kobayashi M, 2002, PHYS REV B, V66, DOI 10.1103/PhysRevB.66.174516 ; LANDAU LD, 1987, STAT PHYS 2 ; Lopatin AV, 2002, PHYS REV LETT, V88, DOI 10.1103/PhysRevLett.88.235503 ; MENG HF, THESIS ; Navez P, 2007, APPL PHYS B-LASERS O, V86, P395, DOI 10.1007/s00340-006-2527-0 ; Nepomnyashchy Y. A., 1978, SOV PHYS JETP, V48, P493 ; Nozieres P., 1990, THEORY QUANTUM LIQUI, VII ; Popov V N, 1983, FUNCTIONAL INTEGRALS ; Shi Hua, 1998, Physics Reports, V304, DOI 10.1016/S0370-1573(98)00015-5 ; Yukalov VI, 2007, PHYS REV A, V75, DOI 10.1103/PhysRevA.75.023619 ; Zobay O, 2006, PHYS REV A, V73, DOI 10.1103/PhysRevA.73.023616},
doi = {10.1103/PhysRevA.75.063619},
groups = {public},
interhash = {f8b380cff6c10564cac20b9d99e5b687},
intrahash = {4147d421f0fe1ca83c54a164c78750f9},
journal = {Physical Review A},
keywords = {GAS},
month = {#jun#},
nr = {25},
number = 6,
pages = 063619,
sn = {1050-2947},
tc = {21},
timestamp = {2012-12-07T18:53:37.000+0100},
title = {Thermodynamics of a Bose-Einstein condensate with weak disorder},
username = {jabreftest},
ut = {WOS:000247624300162},
volume = 75,
wc = {Optics; Physics, Atomic, Molecular & Chemical},
year = 2007,
z9 = {21}
}