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See, e.g
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Lee, P.A.1
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10
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33644627536
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2 symmetry of its singlet order parameter
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see [15]
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2 symmetry of its singlet order parameter; see [15].
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54
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B. Gorshunov P. Haas T. Rõõm M. Dressel T. Vuletić B. Korin-Hamzić S. Tomić J. Akimitsu T. Nagata Phys. Rev. B 66 2002 060508(R)
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Gorshunov, B.1
Haas, P.2
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Dressel, M.4
Vuletić, T.5
Korin-Hamzić, B.6
Tomić, S.7
Akimitsu, J.8
Nagata, T.9
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T. Vuletić B. Korin-Hamzić S. Tomić B. Gorshunov P. Haas T. Rõõm M. Dressel J. Akimitsu T. Sasaki T. Nagata Phys. Rev. Lett. 90 2003 257002
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Phys. Rev. Lett.
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Vuletić, T.1
Korin-Hamzić, B.2
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Gorshunov, B.4
Haas, P.5
Rõõm, T.6
Dressel, M.7
Akimitsu, J.8
Sasaki, T.9
Nagata, T.10
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T. Vuletić T. Ivek B. Korin-Hamzić S. Tomić B. Gorshunov P. Haas M. Dressel J. Akimitsu T. Sasaki T. Nagata Phys. Rev. B 71 2005 012508
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Phys. Rev. B
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Vuletić, T.1
Ivek, T.2
Korin-Hamzić, B.3
Tomić, S.4
Gorshunov, B.5
Haas, P.6
Dressel, M.7
Akimitsu, J.8
Sasaki, T.9
Nagata, T.10
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8344287059
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P. Abbamonte G. Blumberg A. Rusydi A. Gozar P.G. Evans T. Siegrist L. Venema H. Eisaki E.D. Isaacs G.A. Sawatzky Nature 431 2004 1078
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(2004)
Nature
, vol.431
, pp. 1078
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Abbamonte, P.1
Blumberg, G.2
Rusydi, A.3
Gozar, A.4
Evans, P.G.5
Siegrist, T.6
Venema, L.7
Eisaki, H.8
Isaacs, E.D.9
Sawatzky, G.A.10
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60
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0004300713
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See, e.g., K.H. Bennemann J.B. Ketterson, Springer
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See, e.g., E.W. Carlson V.J. Emery S.A. Kivelson D. Orgad K.H. Bennemann J.B. Ketterson The Physics of Conventional and Unconventional Superconductors vol. II 2004 Springer
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(2004)
The Physics of Conventional and Unconventional Superconductors
, vol.2
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Carlson, E.W.1
Emery, V.J.2
Kivelson, S.A.3
Orgad, D.4
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61
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33644618662
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For a discussion of this point, see [20] and references therein
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For a discussion of this point, see [20] and references therein.
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66
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0003900730
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Field Theories for Low-Dimensional Condensed Matter Systems: Spin Systems and Strongly Correlated Electrons
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G. Morandi P. Sodano A. Tagliacozzo V. Tognetti, Springer, New York
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H.J. Schulz G. Cuniberti P. Pieri G. Morandi P. Sodano A. Tagliacozzo V. Tognetti Field Theories for Low-Dimensional Condensed Matter Systems: Spin Systems and Strongly Correlated Electrons 2000 Springer New York
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(2000)
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Schulz, H.J.1
Cuniberti, G.2
Pieri, P.3
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69
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33644611640
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Available from
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(a) D. Sénéchal. Available from: .
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Sénéchal, D.1
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72
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33644626761
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The names D-Mott and S-Mott were introduced in [58]. Note that in [39] the D-Mott and S-Mott phase were referred to as the rung singlet and site singlet phase, respectively
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The names D-Mott and S-Mott were introduced in [58]. Note that in [39] the D-Mott and S-Mott phase were referred to as the rung singlet and site singlet phase, respectively.
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81
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33644630540
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The "Mott" in the name "doped D-Mott phase" is not meant to imply that the phase that results when doping the D-Mott phase is necessarily insulating. Whether or not the various rationally doped phases are insulating is one of the central questions discussed in this paper
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The "Mott" in the name "doped D-Mott phase" is not meant to imply that the phase that results when doping the D-Mott phase is necessarily insulating. Whether or not the various rationally doped phases are insulating is one of the central questions discussed in this paper.
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83
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33644626616
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i 〉
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i〉.
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-
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84
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33644625547
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y would be the associated momentum operator; hence the suggestive notation
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y would be the associated momentum operator; hence the suggestive notation.
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-
-
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86
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33644615996
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2q agrees in all cases
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2q agrees in all cases.
-
-
-
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87
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33644625255
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F2 in the continuum model away from half-filling. Following previous treatments, we assume that this term is irrelevant, at least for sufficiently weak dopings
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F2 in the continuum model away from half-filling. Following previous treatments, we assume that this term is irrelevant, at least for sufficiently weak dopings.
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-
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88
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33644629655
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c [45]
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c [45].
-
-
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92
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33644630130
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F = 2pi;(1 - δ) is expected to be exact. This suggests that the conclusions regarding the basic-Umklapp interaction should hold more generally. This should also include the order-of-magnitude estimate 1/δ for the length scale signifying the crossover from insulating behavior at shorter length scales to metallic behavior at longer length scales
-
F = 2pi;(1 - δ) is expected to be exact. This suggests that the conclusions regarding the basic-Umklapp interaction should hold more generally. This should also include the order-of-magnitude estimate 1/δ for the length scale signifying the crossover from insulating behavior at shorter length scales to metallic behavior at longer length scales.
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97
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33644617652
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We note that by choosing a much smaller value of the fitting parameter b in Fig. 17, the fit of the current could have been much improved, but the density oscillations in the analytical curve would have been smaller than in the numerical curve, which would not be consistent with our picture of the role of quantum fluctuations
-
We note that by choosing a much smaller value of the fitting parameter b in Fig. 17, the fit of the current could have been much improved, but the density oscillations in the analytical curve would have been smaller than in the numerical curve, which would not be consistent with our picture of the role of quantum fluctuations.
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98
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33644629382
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private communication
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B.J. Powell, private communication.
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Powell, B.J.1
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106
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33644613988
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private communication
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I.A. Gruzberg, private communication.
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Gruzberg, I.A.1
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110
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33644618379
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2
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2.
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