-
4
-
-
0002301098
-
-
Springer, Berlin
-
E. K. U. Gross, J. F. Dobson, and M. Petersilka, in Density Functional Theory II, edited by R.F. Nalewajski, Vol. 181 of Topics in Current Chemistry, (Springer, Berlin, 1996), p. 81.
-
(1996)
Density Functional Theory II, edited by R.F. Nalewajski, Vol. 181 of Topics in Current Chemistry
, pp. 81
-
-
Gross, E.K.U.1
Dobson, J.F.2
Petersilka, M.3
-
7
-
-
85038321089
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a more general form, TDFT deals with many-body systems evolving under the influence of time-dependent potentials (formula presented) of arbitrary strength (see Refs. 1, 3, 4 and 6)
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In a more general form, TDFT deals with many-body systems evolving under the influence of time-dependent potentials (formula presented) of arbitrary strength (see Refs. 1, 3, 4 and 6).
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8
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85038292939
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Strictly speaking, the Runge-Gross proof does not apply to adiabatically switched-on periodic potentials such as the ones employed in linear response theory. There are known examples9 of two different periodic potentials producing the same linear response in a finite system. However, such pathologies are expected to disappear10 in extended systems, such as the ones considered in this paper
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Strictly speaking, the Runge-Gross proof does not apply to adiabatically switched-on periodic potentials such as the ones employed in linear response theory. There are known examples9 of two different periodic potentials producing the same linear response in a finite system. However, such pathologies are expected to disappear10 in extended systems, such as the ones considered in this paper.
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12
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85038325801
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We take the point of view that the static xc potential can be adequately treated in one of the existing approximations, e.g., the static LDA. The Kohn-Sham response function can then be constructed in the standard way from the eigenfunctions and eigenvalues of the static Kohn-Sham problem
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We take the point of view that the static xc potential can be adequately treated in one of the existing approximations, e.g., the static LDA. The Kohn-Sham response function can then be constructed in the standard way from the eigenfunctions and eigenvalues of the static Kohn-Sham problem.
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19
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3343023108
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S.J.A. van Gisbergen, P.R.T. Schipper, O.V. Gritsenko, E.J. Baerends, J.G. Snijders, B. Champagne, andB. Kirtman, Phys. Rev. Lett. 83, 694 (1999).
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 694
-
-
Van Gisbergen, S.J.A.1
Schipper, P.R.T.2
Gritsenko, O.V.3
Baerends, E.J.4
Snijders, J.G.5
Champagne, B.6
-
20
-
-
0000621478
-
-
S.J.A. van Gisbergen, F. Kootstra, P.R.T. Schipper, O.V. Gritsenko, J.G. Snijders, andE.J. Baerends, Phys. Rev. A 57, 2556 (1998).
-
(1998)
Phys. Rev. A
, vol.57
, pp. 2556
-
-
Van Gisbergen, S.J.A.1
Kootstra, F.2
Schipper, P.R.T.3
Gritsenko, O.V.4
Snijders, J.G.5
-
22
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85038336149
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It is often stated, not quite accurately, that the Gross-Kohn approximation reduces to the ALDA in the (formula presented) limit. In fact, it turns out that (formula presented), as pointed out in Ref. 37. The Gross-Kohn interpolation formula for (formula presented) does, however, reduce to the ALDA for (formula presented)
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It is often stated, not quite accurately, that the Gross-Kohn approximation reduces to the ALDA in the (formula presented) limit. In fact, it turns out that (formula presented), as pointed out in Ref. 37. The Gross-Kohn interpolation formula for (formula presented) does, however, reduce to the ALDA for (formula presented).
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23
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36149008601
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W. Kohn, Phys. Rev. 123, 1242 (1961);
-
(1961)
Phys. Rev.
, vol.123
, pp. 1242
-
-
Kohn, W.1
-
25
-
-
0000972011
-
-
Phys. Rev. BL. Brey, J. Dempsey, N.F. Johnson, andB.I. Halperin, 42, 1240 (1990);
-
(1990)
Phys. Rev. B
, vol.42
, pp. 1240
-
-
Brey, L.1
Dempsey, J.2
Johnson, N.F.3
-
31
-
-
85038340365
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The factor (formula presented) that usually multiplies the interaction (formula presented) has been absorbed in the vector potential
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The factor (formula presented) that usually multiplies the interaction (formula presented) has been absorbed in the vector potential.
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32
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0001030724
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The generalized Runge-Gross (RG) theorem concerning the uniqueness of (formula presented) is in fact more easily proved than the original RG theorem,1
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The generalized Runge-Gross (RG) theorem concerning the uniqueness of (formula presented) is in fact more easily proved than the original RG theorem,1 seeS.K. Ghosh and A.K. Dhara, Phys. Rev. A 38, 1149 (1988).
-
(1988)
Phys. Rev. A
, vol.38
, pp. 1149
-
-
Ghosh, S.K.1
Dhara, A.K.2
-
37
-
-
0035898601
-
-
J.B. Williams, M.S. Sherwin, K.D. Maranowski, andA.C. Gossard, Phys. Rev. Lett. 87, 037401 (2001).
-
(2001)
Phys. Rev. Lett.
, vol.87
, pp. 37401
-
-
Williams, J.B.1
Sherwin, M.S.2
Maranowski, K.D.3
-
55
-
-
0008629560
-
-
C.L. Cates, G. Briceño, M.S. Sherwin, K.D. Maranowski, K. Campman, andA.C. Gossard, Physica E (Amsterdam) 2, 463 (1998).
-
(1998)
Physica E (Amsterdam)
, vol.2
, pp. 463
-
-
Cates, C.L.1
Briceño, G.2
Sherwin, M.S.3
Maranowski, K.D.4
Campman, K.5
-
56
-
-
0028304539
-
-
J. Faist, F. Capasso, D.L. Sivco, C. Sirtori, A.L. Hutchinson, andA.Y. Cho, Science 264, 553 (1994).
-
(1994)
Science
, vol.264
, pp. 553
-
-
Faist, J.1
Capasso, F.2
Sivco, D.L.3
Sirtori, C.4
Hutchinson, A.L.5
-
58
-
-
5644250816
-
-
K.L. Campman, H. Schmidt, A. Imamoglu, andA.C. Gossard, Appl. Phys. Lett. 69, 2554 (1996).
-
(1996)
Appl. Phys. Lett.
, vol.69
, pp. 2554
-
-
Campman, K.L.1
Schmidt, H.2
Imamoglu, A.3
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