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33847690144
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K. S. Novoselov, A. K. Geim, S. V. Morozov, D. Jiang, M. I. Katsnelson, I. V. Grigorieva, S. V. Dubonos, and A. A. Firsov, Nature (London) NATUAS 0028-0836 10.1038/nature04233 438, 197 (2005).
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Nature (London)
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NATUAS 0028-0836 10.1038/nature04235
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Y. Zhang, Y. W. Tan, H. L. Stormer, and P. Kim, Nature (London) NATUAS 0028-0836 10.1038/nature04235 438, 201 (2005).
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Nature (London)
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Zhang, Y.1
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D. V. Khveshchenko and H. Leal, Nucl. Phys. B NUPBBO 0550-3213 10.1016/j.nuclphysb.2004.03.020 687, 323 (2004);
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D. T. Son, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.75.235423 75, 235423 (2007).
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Phys. Rev. B
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Son, D.T.1
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0003430317
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For a general construction of the terms compatible with the lattice symmetries, see Wiley, New York
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For a general construction of the terms compatible with the lattice symmetries, see G. L. Bir and G. E. Pikus, Symmetry and Strain-Induced Effects in Semiconductors (Wiley, New York, 1974).
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Symmetry and Strain-Induced Effects in Semiconductors
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Bir, G.L.1
Pikus, G.E.2
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12
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33845242289
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We use parametrization as in PRLTAO 0031-9007 10.1103/PhysRevLett.96. 236801
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We use parametrization as in I. L. Aleiner and K. B. Efetov, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.96.236801 97, 236801 (2006).
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J. M. Kosterlitz and D. J. Thouless, J. Phys. C JPSOAW 0022-3719 10.1088/0022-3719/5/11/002 5, L124 (1972);
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J. M. Kosterlitz and D. J. Thouless, J. Phys. C JPSOAW 0022-3719 10.1088/0022-3719/6/7/010 6, 1181 (1973).
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Kosterlitz, J.M.1
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18
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0004056428
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In the mean-field picture, the existence of such lines and the points where three continuous phase transitions intersect is not possible [see Sec. 150 of Pergamon, New York
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In the mean-field picture, the existence of such lines and the points where three continuous phase transitions intersect is not possible [see Sec. 150 of L. D. Landau and E. M. Lifshits, Statistical Physics (Pergamon, New York, 1986)], and the critical line B1 - B1′ [see Fig. 5] becomes either the first order phase transition line or splits into two second order phase transition lines. The existence of this line is a consequence of the fluctuations, making the vortex operator cos 2π hs vanish.
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(1986)
Statistical Physics
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Landau, L.D.1
Lifshits, E.M.2
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20
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34547261925
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See, e.g., PRLTAO 0031-9007 10.1103/PhysRevLett.98.197403
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See, e.g., Z. Jiang, E. A. Henriksen, L. C. Tung, Y.-J. Wang, M. E. Schwartz, M. Y. Han, P. Kim, and H. L. Stormer, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.98.197403 98, 197403 (2007);
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Jiang, Z.1
Henriksen, E.A.2
Tung, L.C.3
Wang, Y.-J.4
Schwartz, M.E.5
Han, M.Y.6
Kim, P.7
Stormer, H.L.8
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21
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34548444217
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PRBMDO 0163-1829 10.1103/PhysRevB.76.081406
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R. S. Deacon, K.-C. Chuang, R. J. Nicholas, K. S. Novoselov, and A. K. Geim, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.76.081406 76, 081406 (R) (2007).
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Geim, A.K.5
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22
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36148960352
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Formula (5.9) for rc R was first obtained by
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Formula (5.9) for rc R was first obtained by I. L. Aleiner and V. I. Falko (unpublished).
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Aleiner, I.L.1
Falko, V.I.2
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23
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34147183208
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PRLTAO 0031-9007 10.1103/PhysRevLett.98.156801
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D. A. Abanin, P. A. Lee, and L. S. Levitov, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.98.156801 98, 156801 (2007).
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Phys. Rev. Lett.
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Abanin, D.A.1
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Levitov, L.S.3
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24
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34247394616
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PRBMDO 0163-1829 10.1103/PhysRevB.75.165411
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I. F. Herbut, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.75.165411 75, 165411 (2007).
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Phys. Rev. B
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Herbut, I.F.1
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25
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33749501025
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PRLTAO 0031-9007 10.1103/PhysRevLett.97.146805
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E. McCann, K. Kechedzhi, V. I. Fal'ko, H. Suzuura, T. Ando, and B. L. Altshuler, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.97.146805 97, 146805 (2006).
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McCann, E.1
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Suzuura, H.4
Ando, T.5
Altshuler, B.L.6
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26
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33845532235
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Detailed calculation of the polarization operator at finite doping can be found in NJOPFM 1367-2630 10.1088/1367-2630/8/12/318
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Detailed calculation of the polarization operator at finite doping can be found in B. Wunsch, T. Stauber, F. Sols, and F. Guinea, New J. Phys. NJOPFM 1367-2630 10.1088/1367-2630/8/12/318 8, 318 (2006). For our purposes, it is important only that Π (0,q) does not depend on the wave vector at all for q<2 kF.
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(2006)
New J. Phys.
, vol.8
, pp. 318
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Wunsch, B.1
Stauber, T.2
Sols, F.3
Guinea, F.4
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27
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36148943064
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This idea belongs to
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This idea belongs to I. Zaliznyak (private communication).
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Zaliznyak, I.1
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