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024 7 _ |2 DOI
|a 10.1103/PhysRevLett.106.236805
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|a 2128/7302
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041 _ _ |a eng
082 _ _ |a 550
084 _ _ |2 WoS
|a Physics, Multidisciplinary
100 1 _ |0 P:(DE-HGF)0
|a Wehling, T. O.
|b 0
245 _ _ |a Strength of Effective Coulomb Interactions in Graphene and Graphite
260 _ _ |a College Park, Md.
|b APS
|c 2011
300 _ _ |a 236805
336 7 _ |a Journal Article
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336 7 _ |a article
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440 _ 0 |0 4925
|a Physical Review Letters
|v 106
|x 0031-9007
|y 23
500 _ _ |3 POF3_Assignment on 2016-02-29
500 _ _ |a Financial support by the Deutsche Forschungsgemeinschaft through FOR-912, FOR-1346, SFB 668, SPP 1145, SPP 1459, and FOM (The Netherlands) is acknowledged. T. O. W. is grateful to FZ Julich for hospitality during the visit, when parts of this work were conceived. One of us, S. B., thanks Achim Rosch for fruitful discussions.
520 _ _ |a To obtain an effective many-body model of graphene and related materials from first principles we calculate the partially screened frequency dependent Coulomb interaction. In graphene, the effective on-site (Hubbard) interaction is U-00 = 9.3 eV in close vicinity to the critical value separating conducting graphene from an insulating phase emphasizing the importance of nonlocal Coulomb terms. The nearest-neighbor Coulomb interaction strength is computed to U-01 = 5.5 eV. In the long-wavelength limit, we find the effective background dielectric constant of graphite to be is an element of = 2.5 in very good agreement with experiment.
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|a Friedrich, C.
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|a Lichtenstein, A. I.
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|a Katsnelson, M. I.
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|a Blügel, S.
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|t Physical review letters
|v 106
|x 0031-9007
|y 2011
856 7 _ |u http://dx.doi.org/10.1103/PhysRevLett.106.236805
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