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4
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85038912509
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C. J. Halboth, Ph.D. thesis, Shaker-Verlag, Aachen, 1999
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C. J. Halboth, Ph.D. thesis, Shaker-Verlag, Aachen, 1999.
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7
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85038901642
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C. Honerkamp, Ph.D. thesis, ETH Zürich, 2000
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C. Honerkamp, Ph.D. thesis, ETH Zürich, 2000.
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8
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0035131075
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C. Honerkamp, M. Salmhofer, N. Furukawa, and T.M. Rice, Phys. Rev. B 63, 045114 (2001);
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(2001)
Phys. Rev. B
, vol.63
, pp. 45114
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Honerkamp, C.1
Salmhofer, M.2
Furukawa, N.3
Rice, T.M.4
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10
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85038959892
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cond-mat/0103172 (unpublished)
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C. Honerkamp, cond-mat/0103172 (unpublished).
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Honerkamp, C.1
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27
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85038894957
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J. Zinn-Justin, Quantum Field Theory and Critical Phenomena (Clarendon Press, Oxford, 1989); M. Le Ballac, Quantum and Statistical Field Theory (Clarendon Press, Oxford, 1991)
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J. Zinn-Justin, Quantum Field Theory and Critical Phenomena (Clarendon Press, Oxford, 1989); M. Le Ballac, Quantum and Statistical Field Theory (Clarendon Press, Oxford, 1991).
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29
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85038959456
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If (Formula presented) lies outside a closed Fermi surface (as shown in Fig. 11), then the mapping (Formula presented) defined by (Formula presented) yields a unique (Formula presented) for each (Formula presented). On the other hand, if (Formula presented) lies inside a closed Fermi surface, then (Formula presented) may have more than one solution (Formula presented) In this case we choose the solution which minimizes (Formula presented)
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If (Formula presented) lies outside a closed Fermi surface (as shown in Fig. 11), then the mapping (Formula presented) defined by (Formula presented) yields a unique (Formula presented) for each (Formula presented). On the other hand, if (Formula presented) lies inside a closed Fermi surface, then (Formula presented) may have more than one solution (Formula presented) In this case we choose the solution which minimizes (Formula presented).
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32
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85038965646
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J. W. Negele and H. Orland, Quantum Many-Particle Systems, (Addison-Wesley, Redwood City, CA, 1988)
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J. W. Negele and H. Orland, Quantum Many-Particle Systems, (Addison-Wesley, Redwood City, CA, 1988).
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37
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85038912455
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We introduce (Formula presented) because then the bosonic version of the exact flow equations of Sec. II can be simply obtained by replacing (Formula presented)
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We introduce (Formula presented) because then the bosonic version of the exact flow equations of Sec. II can be simply obtained by replacing (Formula presented).
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38
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85038938174
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Although we use a different notation, our Eq. (2.16) is equivalent to the flow equation for the Legendre effective action given in Refs. 4 and 5. We have adopted the same notation as Ref. 16 to emphasize the analogy with (Formula presented) theory
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Although we use a different notation, our Eq. (2.16) is equivalent to the flow equation for the Legendre effective action given in Refs. 4 and 5. We have adopted the same notation as Ref. 16 to emphasize the analogy with (Formula presented) theory.
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53
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85038908498
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cond-mat/0104576 (unpublished)
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A. Ferraz, cond-mat/0104576 (unpublished).
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Ferraz, A.1
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