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A. Nepomnyashchy and Y. A. Nepomnyashchy, JETP Letters 21, 1 (1975); Y. A. Nepomnyashchy and A. Nepomnyashchy, Sov. Phys. JETP 48, 493 (1978); Y. A. Nepomnyashchy, ibid. 58, 6611 (1983); Phys. Rev. B 46, 6611 (1992).
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A. Nepomnyashchy and Y. A. Nepomnyashchy, JETP Letters 21, 1 (1975); Y. A. Nepomnyashchy and A. Nepomnyashchy, Sov. Phys. JETP 48, 493 (1978); Y. A. Nepomnyashchy, ibid. 58, 6611 (1983); Phys. Rev. B 46, 6611 (1992).
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C. Castellani, C. Di Castro, F. Pistolesi, and G. C. Strinati, Phys. Rev. Lett. 78, 1612 (1997).
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W. Metzner and C. Di Castro, Phys. Rev. B 47, 16 107 (1993); W. Metzner, C. Castellani, and C. Di Castro, Adv. Phys. 47, 317 (1998).
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W. Metzner and C. Di Castro, Phys. Rev. B 47, 16 107 (1993); W. Metzner, C. Castellani, and C. Di Castro, Adv. Phys. 47, 317 (1998).
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edited by Vincent Rivasseau (Springer Verlag, New York)
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G. Benfatto, in Constructive Results in Field Theory, Statistical Mechanics, and Condensed Matter Physics, edited by Vincent Rivasseau (Springer Verlag, New York, 1994). See also G. Benfatto and G. Gallavotti, Renormalization Group (Princeton University Press, Princeton, 1995).
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G. Benfatto, in Constructive Results in Field Theory, Statistical Mechanics, and Condensed Matter Physics, edited by Vincent Rivasseau (Springer Verlag, New York, 1994). See also G. Benfatto and G. Gallavotti, Renormalization Group (Princeton University Press, Princeton, 1995).
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33646637234
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cond-mat/0305138 (unpublished)
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For a recent review on field theory methods for interacting boson gas see, for instance, J. O. Andersen, cond-mat/0305138 (unpublished).
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Andersen, J.O.1
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0001358131
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A neat application of the loop expansion has been used recently to calculate the quantum corrections at two-loop order for the ground-state energy of a condensate Bose gas: E. Braaten and A. Nieto, Eur. Phys. J. B 11, 143 (1999).
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Eur. Phys. J. B
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Braaten, E.1
Nieto, A.2
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note
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The noninteracting boson system, on the contrary, with fixed chemical potential, is not well defined (as at T=0 and μ<0 the system contains no particle). As a consequence, the perturbative expansion is not well defined. On the other hand, the organization of classes of diagrams on the basis of the IR divergences-as we do-seems to be a well-defined procedure since it bypasses the expansion in the bare potential.
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Monomials linear in the frequency and containing fields of the same type vanish identically, as they represent total derivatives in the action.
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note
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One can show by power counting that in the variables phase and modulus all running couplings are irrelevant. This is equivalent to stating that no IR divergences appear in the theory.
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edited by C. Domb and M. S. Green (Academic, New York)
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See, e.g., Phase Transitions and Critical Phenomena, edited by C. Domb and M. S. Green (Academic, New York, 1976), Vol. VI.
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Phase Transitions and Critical Phenomena
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