-
1
-
-
7444220645
-
Electric field in atomically thin carbon films
-
DOI 10.1126/science.1102896
-
K. S. Novoselov, A. K. Geim, S. V. Morozov, D. Jiang, Y. Zhang, S. V. Dubonos, I. V. Grigorieva, and A. A. Firsov, Science SCIEAS 0036-8075 10.1126/science.1102896 306, 666 (2004). (Pubitemid 39440910)
-
(2004)
Science
, vol.306
, Issue.5696
, pp. 666-669
-
-
Novoselov, K.S.1
Geim, A.K.2
Morozov, S.V.3
Jiang, D.4
Zhang, Y.5
Dubonos, S.V.6
Grigorieva, I.V.7
Firsov, A.A.8
-
2
-
-
59949098337
-
-
RMPHAT 0034-6861 10.1103/RevModPhys.81.109
-
A. H. Castro Neto, F. Guinea, N. M. R. Peres, K. S. Novoselov, and A. K. Geim, Rev. Mod. Phys. RMPHAT 0034-6861 10.1103/RevModPhys.81.109 81, 109 (2009).
-
(2009)
Rev. Mod. Phys.
, vol.81
, pp. 109
-
-
Castro Neto, A.H.1
Guinea, F.2
Peres, N.M.R.3
Novoselov, K.S.4
Geim, A.K.5
-
3
-
-
47749150628
-
Measurement of the elastic properties and intrinsic strength of monolayer graphene
-
DOI 10.1126/science.1157996
-
C. Lee, X. Weil, J. W. Kysar, and J. Hone, Science SCIEAS 0036-8075 10.1126/science.1157996 321, 385 (2008). (Pubitemid 352029970)
-
(2008)
Science
, vol.321
, Issue.5887
, pp. 385-388
-
-
Lee, C.1
Wei, X.2
Kysar, J.W.3
Hone, J.4
-
4
-
-
27744475163
-
Experimental observation of the quantum Hall effect and Berry's phase in graphene
-
DOI 10.1038/nature04235, PII N04235
-
Y. Zhang, Y.-W. Tan, H. L. Stormer, and P. Kim, Nature (London) NATUAS 0028-0836 10.1038/nature04235 438, 201 (2005). (Pubitemid 41599868)
-
(2005)
Nature
, vol.438
, Issue.7065
, pp. 201-204
-
-
Zhang, Y.1
Tan, Y.-W.2
Stormer, H.L.3
Kim, P.4
-
5
-
-
27744534165
-
Two-dimensional gas of massless Dirac fermions in graphene
-
DOI 10.1038/nature04233, PII N04233
-
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). (Pubitemid 41599867)
-
(2005)
Nature
, vol.438
, Issue.7065
, pp. 197-200
-
-
Novoselov, K.S.1
Geim, A.K.2
Morozov, S.V.3
Jiang, D.4
Katsnelson, M.I.5
Grigorieva, I.V.6
Dubonos, S.V.7
Firsov, A.A.8
-
6
-
-
0030492538
-
-
JUPSAU 0031-9015 10.1143/JPSJ.65.1920
-
M. Fujita, K. Wakabayashi, K. Nakada, and K. Kusakabe, J. Phys. Soc. Jpn. JUPSAU 0031-9015 10.1143/JPSJ.65.1920 65, 1920 (1996).
-
(1996)
J. Phys. Soc. Jpn.
, vol.65
, pp. 1920
-
-
Fujita, M.1
Wakabayashi, K.2
Nakada, K.3
Kusakabe, K.4
-
7
-
-
33751348065
-
Energy gaps in graphene nanoribbons
-
DOI 10.1103/PhysRevLett.97.216803
-
Y.-W. Son, M. L. Cohen, and S. G. Louie, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.97.216803 97, 216803 (2006). (Pubitemid 44808139)
-
(2006)
Physical Review Letters
, vol.97
, Issue.21
, pp. 216803
-
-
Son, Y.-W.1
Cohen, M.L.2
Louie, S.G.3
-
9
-
-
68949149415
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.79.235433
-
J. Jung and A. H. MacDonald, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.79.235433 79, 235433 (2009).
-
(2009)
Phys. Rev. B
, vol.79
, pp. 235433
-
-
Jung, J.1
MacDonald, A.H.2
-
10
-
-
77955077835
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.81.115416
-
H. Feldner, Z. Y. Meng, A. Honecker, D. Cabra, S. Wessel, and F. F. Assaad, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.81.115416 81, 115416 (2010).
-
(2010)
Phys. Rev. B
, vol.81
, pp. 115416
-
-
Feldner, H.1
Meng, Z.Y.2
Honecker, A.3
Cabra, D.4
Wessel, S.5
Assaad, F.F.6
-
11
-
-
79961109395
-
-
H. Feldner, Z. Y. Meng, T. C. Lang, F. F. Assaad, S. Wessel, and A. Honecker, e-print arXiv: 1101.1882 (to be published)
-
H. Feldner, Z. Y. Meng, T. C. Lang, F. F. Assaad, S. Wessel, and A. Honecker, e-print arXiv: 1101.1882 (to be published).
-
-
-
-
12
-
-
12544254704
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.68.035432
-
T. Hikihara, X. Hu, H.-H. Lin, and C.-Y. Mou, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.68.035432 68, 035432 (2003).
-
(2003)
Phys. Rev. B
, vol.68
, pp. 035432
-
-
Hikihara, T.1
Hu, X.2
Lin, H.-H.3
Mou, C.-Y.4
-
13
-
-
77957560287
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.82.085422
-
M. J. Schmidt and D. Loss, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.82.085422 82, 085422 (2010).
-
(2010)
Phys. Rev. B
, vol.82
, pp. 085422
-
-
Schmidt, M.J.1
Loss, D.2
-
14
-
-
36149025693
-
-
PHRVAO 0031-899X 10.1103/PhysRev.125.164
-
E. Lieb and D. Mattis, Phys. Rev. PHRVAO 0031-899X 10.1103/PhysRev.125. 164 125, 164 (1962).
-
(1962)
Phys. Rev.
, vol.125
, pp. 164
-
-
Lieb, E.1
Mattis, D.2
-
16
-
-
12044251032
-
Correlated electrons in high-temperature superconductors
-
DOI 10.1103/RevModPhys.66.763
-
E. Dagotto, Rev. Mod. Phys. RMPHAT 0034-6861 10.1103/RevModPhys.66.763 66, 763 (1994). (Pubitemid 24821628)
-
(1994)
Reviews of Modern Physics
, vol.66
, Issue.3
, pp. 763
-
-
Dagotto, E.1
-
17
-
-
79961106246
-
-
D. Sénéchal, e-print arXiv: 0806.2690 (to be published)
-
D. Sénéchal, e-print arXiv: 0806.2690 (to be published).
-
-
-
-
18
-
-
79961103961
-
-
z=L/6-2 and L/3 filling, we were able to calculate the ground-state energy of an edge with length L=180 with a Hilbert space dimension of only 26 580. In this case we were limited only by the 64-bit limit of the internal storage of the basis vectors and longer edges are in principle accessible by a modification of our code
-
z=L/6-2 and L/3 filling, we were able to calculate the ground-state energy of an edge with length L=180 with a Hilbert space dimension of only 26, 580. In this case we were limited only by the 64-bit limit of the internal storage of the basis vectors and longer edges are in principle accessible by a modification of our code.
-
-
-
-
19
-
-
79961125170
-
-
It is only important to assume that this energy scale is large enough so that the restriction to the zero-energy sector of H is well justified. The validity of this assumption has been checked in Ref. 13
-
It is only important to assume that this energy scale is large enough so that the restriction to the zero-energy sector of H is well justified. The validity of this assumption has been checked in Ref. 13.
-
-
-
-
20
-
-
77955397600
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.81.165439
-
M. J. Schmidt and D. Loss, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.81.165439 81, 165439 (2010).
-
(2010)
Phys. Rev. B
, vol.81
, pp. 165439
-
-
Schmidt, M.J.1
Loss, D.2
-
21
-
-
79952422000
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.106.100403
-
M. Hohenadler, T. C. Lang, and F. F. Assaad, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.106.100403 106, 100403 (2011).
-
(2011)
Phys. Rev. Lett.
, vol.106
, pp. 100403
-
-
Hohenadler, M.1
Lang, T.C.2
Assaad, F.F.3
-
23
-
-
79961101534
-
-
F,0), which is a consequence of the origin of Γ in the 2D honeycomb Hubbard model (see Ref. 13)
-
F, 0), which is a consequence of the origin of Γ in the 2D honeycomb Hubbard model (see Ref. 13).
-
-
-
-
24
-
-
79961103700
-
-
M. J. Schmidt (2011)
-
M. J. Schmidt (2011).
-
-
-
-
25
-
-
79961118760
-
-
An edge with L unit cells in length corresponds to only L/3k-space points in the reduced Brillouin zone in which the edge states are defined
-
An edge with L unit cells in length corresponds to only L / 3 k -space points in the reduced Brillouin zone in which the edge states are defined.
-
-
-
-
26
-
-
79961120926
-
-
We have checked that the linearization of the single-particle spectrum does not change the results qualitatively
-
We have checked that the linearization of the single-particle spectrum does not change the results qualitatively.
-
-
-
-
27
-
-
79961104799
-
-
Fπ/U=0 corresponds to a pathologic potential in Ref. 14, as it can be reached by U→∞. At this point, all sectors with total spin 0≤S≤Smax are degenerate
-
Fπ/U=0 corresponds to a pathologic potential in Ref. 14, as it can be reached by U → ∞. At this point, all sectors with total spin 0≤S≤ Smax are degenerate.
-
-
-
-
28
-
-
79961122017
-
-
Note that the increase in the interaction vertex for the spin-down electrons with lowered Fermi level is overcompensated by the suppression due to the higher Fermi level of the spin-up electrons, so that in total the interaction is reduced as S grows
-
Note that the increase in the interaction vertex for the spin-down electrons with lowered Fermi level is overcompensated by the suppression due to the higher Fermi level of the spin-up electrons, so that in total the interaction is reduced as S grows.
-
-
-
-
29
-
-
79961103275
-
-
This decrease of 2 in S is due to the contribution of the left- and right-moving branch to the spin-polarization: Each branch contributes one spin flip
-
This decrease of 2 in S is due to the contribution of the left- and right-moving branch to the spin-polarization: Each branch contributes one spin flip.
-
-
-
-
30
-
-
0009933524
-
-
EPJBFY 1434-6028 10.1007/s100510051074
-
S. Daul, Eur. Phys. J. B EPJBFY 1434-6028 10.1007/s100510051074 14, 649 (2000).
-
(2000)
Eur. Phys. J. B
, vol.14
, pp. 649
-
-
Daul, S.1
-
31
-
-
0000733615
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.58.2635
-
S. Daul and R. M. Noack, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.58.2635 58, 2635 (1998).
-
(1998)
Phys. Rev. B
, vol.58
, pp. 2635
-
-
Daul, S.1
Noack, R.M.2
|