-
1
-
-
34250905523
-
-
BLOCH F., Z. Phys., 57 (1929) 545; WIGNER E. P. and SEITZ F., Phys. Rev., 43 (1933) 804.
-
(1929)
Z. Phys.
, vol.57
, pp. 545
-
-
Bloch, F.1
-
4
-
-
0019711815
-
-
See SINGWI K. S. and TOSI M. P., Solid State Phys., 36 (1981) 177 and YARLAGADDA S. and GIULIANI G. F., Phys. Rev. B, 38 (1988) 10966 for examples of such calculations in three and two space dimensions, respectively.
-
(1981)
Solid State Phys.
, vol.36
, pp. 177
-
-
Singwi, K.S.1
Tosi, M.P.2
-
5
-
-
0007289456
-
-
for examples of such calculations in three and two space dimensions, respectively
-
See SINGWI K. S. and TOSI M. P., Solid State Phys., 36 (1981) 177 and YARLAGADDA S. and GIULIANI G. F., Phys. Rev. B, 38 (1988) 10966 for examples of such calculations in three and two space dimensions, respectively.
-
(1988)
Phys. Rev. B
, vol.38
, pp. 10966
-
-
Yarlagadda, S.1
Giuliani, G.F.2
-
6
-
-
33744691386
-
-
See, for example, CEPERLEY D. M. and ALDER B. J., Phys. Rev. Lett., 45 (1980) 566; TANATAR B. and CEPERLEY D. M., Phys. Rev. B, 39 (1989) 5005; KWON Y. K., CEPERLEY D. M. and MARTIN R. M., Phys. Rev. B, 50 (1994) 1684; MARONI S., CEPERLEY D. M. and SENATORE G., Phys. Rev. Lett., 75 (1995) 689.
-
(1980)
Phys. Rev. Lett.
, vol.45
, pp. 566
-
-
Ceperley, D.M.1
Alder, B.J.2
-
7
-
-
24244445528
-
-
See, for example, CEPERLEY D. M. and ALDER B. J., Phys. Rev. Lett., 45 (1980) 566; TANATAR B. and CEPERLEY D. M., Phys. Rev. B, 39 (1989) 5005; KWON Y. K., CEPERLEY D. M. and MARTIN R. M., Phys. Rev. B, 50 (1994) 1684; MARONI S., CEPERLEY D. M. and SENATORE G., Phys. Rev. Lett., 75 (1995) 689.
-
(1989)
Phys. Rev. B
, vol.39
, pp. 5005
-
-
Tanatar, B.1
Ceperley, D.M.2
-
8
-
-
0000658959
-
-
See, for example, CEPERLEY D. M. and ALDER B. J., Phys. Rev. Lett., 45 (1980) 566; TANATAR B. and CEPERLEY D. M., Phys. Rev. B, 39 (1989) 5005; KWON Y. K., CEPERLEY D. M. and MARTIN R. M., Phys. Rev. B, 50 (1994) 1684; MARONI S., CEPERLEY D. M. and SENATORE G., Phys. Rev. Lett., 75 (1995) 689.
-
(1994)
Phys. Rev. B
, vol.50
, pp. 1684
-
-
Kwon, Y.K.1
Ceperley, D.M.2
Martin, R.M.3
-
9
-
-
3343017610
-
-
See, for example, CEPERLEY D. M. and ALDER B. J., Phys. Rev. Lett., 45 (1980) 566; TANATAR B. and CEPERLEY D. M., Phys. Rev. B, 39 (1989) 5005; KWON Y. K., CEPERLEY D. M. and MARTIN R. M., Phys. Rev. B, 50 (1994) 1684; MARONI S., CEPERLEY D. M. and SENATORE G., Phys. Rev. Lett., 75 (1995) 689.
-
(1995)
Phys. Rev. Lett.
, vol.75
, pp. 689
-
-
Maroni, S.1
Ceperley, D.M.2
Senatore, G.3
-
11
-
-
0006016757
-
-
For reviews see, e.g., VOIT J., Rep. Prog. Phys., 58 (1995) 97 and SCHULZ H. J., in Mesoscopic Quantum Physics, edited by E. AKKERMANS, G. MONTAMBEAUX, J.-L. PICHARD and J. ZINN-JUSTIN (Elsevier, Amsterdam) 1995.
-
(1995)
Rep. Prog. Phys.
, vol.58
, pp. 97
-
-
Voit, J.1
-
12
-
-
0004266556
-
-
edited by E. AKKERMANS, G. MONTAMBEAUX, J.-L. PICHARD and J. ZINN-JUSTIN (Elsevier, Amsterdam)
-
For reviews see, e.g., VOIT J., Rep. Prog. Phys., 58 (1995) 97 and SCHULZ H. J., in Mesoscopic Quantum Physics, edited by E. AKKERMANS, G. MONTAMBEAUX, J.-L. PICHARD and J. ZINN-JUSTIN (Elsevier, Amsterdam) 1995.
-
(1995)
Mesoscopic Quantum Physics
-
-
Schulz, H.J.1
-
13
-
-
0007217252
-
-
note
-
This property is one consequence of the invariance of the interaction energy under a shift of the many-electron state in momentum space, producing a Drude weight in the conductivity which is independent of interactions.
-
-
-
-
14
-
-
0007336672
-
-
note
-
We are aware of another recent quantum Monte Carlo study of the one-dimensional electron liquid: MALATESTA A., PhD Thesis, University of Trieste (1999) and MALATESTA A. and SENATORE G., in preparation. The focus of this work is on correlation functions of the ID electron liquid.
-
-
-
-
15
-
-
4244007319
-
-
TL parameters have been calculated previously for models which are primarily of theoretical interest, cf. SCHULZ H. J., Phys. Rev. Lett., 64 (1990) 2831; KAWAKAMI N. and YANG S.-K., Phys. Rev. Lett., 65 (1990) 2309; 67 (1991) 2493.
-
(1990)
Phys. Rev. Lett.
, vol.64
, pp. 2831
-
-
Schulz, H.J.1
-
16
-
-
4243190824
-
-
TL parameters have been calculated previously for models which are primarily of theoretical interest, cf. SCHULZ H. J., Phys. Rev. Lett., 64 (1990) 2831; KAWAKAMI N. and YANG S.-K., Phys. Rev. Lett., 65 (1990) 2309; 67 (1991) 2493.
-
(1990)
Phys. Rev. Lett.
, vol.65
, pp. 2309
-
-
Kawakami, N.1
Yang, S.-K.2
-
17
-
-
4243262149
-
-
TL parameters have been calculated previously for models which are primarily of theoretical interest, cf. SCHULZ H. J., Phys. Rev. Lett., 64 (1990) 2831; KAWAKAMI N. and YANG S.-K., Phys. Rev. Lett., 65 (1990) 2309; 67 (1991) 2493.
-
(1991)
Phys. Rev. Lett.
, vol.67
, pp. 2493
-
-
-
18
-
-
0033580273
-
-
BOCKRATH M. et al., Nature, 397 (1999) 598.
-
(1999)
Nature
, vol.397
, pp. 598
-
-
Bockrath, M.1
-
25
-
-
0034138837
-
-
ROTHER M. et al., Physica E, 6 (2000) 551.
-
(2000)
Physica E
, vol.6
, pp. 551
-
-
Rother, M.1
-
26
-
-
0007178040
-
-
and ref. [10] are closely related to those discussed here. Nanotubes, however, have two 1D bands at the Fermi energy, and the short distance cutoff of the Coulomb interaction occurs at the tube diameter, which exceeds the distance between valence electrons
-
The ID electron systems which occur in carbon nanotubes (cf. TANS S. J., et al., Nature, 386 (1997) 474 and ref. [10]) are closely related to those discussed here. Nanotubes, however, have two 1D bands at the Fermi energy, and the short distance cutoff of the Coulomb interaction occurs at the tube diameter, which exceeds the distance between valence electrons (cf. EGGER R. and GOGOLIN A. O., Phys. Rev. Lett., 78 (1997) 5082; Eur. J. B, 3 (1998) 281, and C.L. KANE, FISHER M. P. A. and BALENTS L., Phys. Rev. Lett., 78 (1997) 5086), and thus they are not described by a HEL model.
-
(1997)
Nature
, vol.386
, pp. 474
-
-
Tans, S.J.1
-
27
-
-
3242890572
-
-
The ID electron systems which occur in carbon nanotubes (cf. TANS S. J., et al., Nature, 386 (1997) 474 and ref. [10]) are closely related to those discussed here. Nanotubes, however, have two 1D bands at the Fermi energy, and the short distance cutoff of the Coulomb interaction occurs at the tube diameter, which exceeds the distance between valence electrons (cf. EGGER R. and GOGOLIN A. O., Phys. Rev. Lett., 78 (1997) 5082; Eur. J. B, 3 (1998) 281, and C.L. KANE, FISHER M. P. A. and BALENTS L., Phys. Rev. Lett., 78 (1997) 5086), and thus they are not described by a HEL model.
-
(1997)
Phys. Rev. Lett.
, vol.78
, pp. 5082
-
-
Egger, R.1
Gogolin, A.O.2
-
28
-
-
0007343645
-
-
The ID electron systems which occur in carbon nanotubes (cf. TANS S. J., et al., Nature, 386 (1997) 474 and ref. [10]) are closely related to those discussed here. Nanotubes, however, have two 1D bands at the Fermi energy, and the short distance cutoff of the Coulomb interaction occurs at the tube diameter, which exceeds the distance between valence electrons (cf. EGGER R. and GOGOLIN A. O., Phys. Rev. Lett., 78 (1997) 5082; Eur. J. B, 3 (1998) 281, and C.L. KANE, FISHER M. P. A. and BALENTS L., Phys. Rev. Lett., 78 (1997) 5086), and thus they are not described by a HEL model.
-
(1998)
Eur. J. B
, vol.3
, pp. 281
-
-
-
29
-
-
0031343951
-
-
and thus they are not described by a HEL model
-
The ID electron systems which occur in carbon nanotubes (cf. TANS S. J., et al., Nature, 386 (1997) 474 and ref. [10]) are closely related to those discussed here. Nanotubes, however, have two 1D bands at the Fermi energy, and the short distance cutoff of the Coulomb interaction occurs at the tube diameter, which exceeds the distance between valence electrons (cf. EGGER R. and GOGOLIN A. O., Phys. Rev. Lett., 78 (1997) 5082; Eur. J. B, 3 (1998) 281, and C.L. KANE, FISHER M. P. A. and BALENTS L., Phys. Rev. Lett., 78 (1997) 5086), and thus they are not described by a HEL model.
-
(1997)
Phys. Rev. Lett.
, vol.78
, pp. 5086
-
-
Kane, C.L.1
Fisher, M.P.A.2
Balents, L.3
-
35
-
-
0000511081
-
-
edited by V. J. EMERY (World Scientific, Singapore)
-
SCHULZ H. J., in Correlated Electron Systems, edited by V. J. EMERY (World Scientific, Singapore) 1993, p. 199.
-
(1993)
Correlated Electron Systems
, pp. 199
-
-
Schulz, H.J.1
-
36
-
-
0011402903
-
-
CARDY J. L., Nucl. Phys. B, 270 (1986) 186; BLÖTE H. W. J., CARDY J. L. and NIGHTINGALE M. P., Phys. Rev. Lett., 56 (1986) 742; AFFLECK I., Phys. Rev. Lett., 56 (1986) 746; MIRONOV A. D. and ZABRODIN A. V., Phys. Rev. Lett., 66 (1991) 534.
-
(1986)
Nucl. Phys. B
, vol.270
, pp. 186
-
-
Cardy, J.L.1
-
37
-
-
33744747026
-
-
CARDY J. L., Nucl. Phys. B, 270 (1986) 186; BLÖTE H. W. J., CARDY J. L. and NIGHTINGALE M. P., Phys. Rev. Lett., 56 (1986) 742; AFFLECK I., Phys. Rev. Lett., 56 (1986) 746; MIRONOV A. D. and ZABRODIN A. V., Phys. Rev. Lett., 66 (1991) 534.
-
(1986)
Phys. Rev. Lett.
, vol.56
, pp. 742
-
-
Blöte, H.W.J.1
Cardy, J.L.2
Nightingale, M.P.3
-
38
-
-
0001487832
-
-
CARDY J. L., Nucl. Phys. B, 270 (1986) 186; BLÖTE H. W. J., CARDY J. L. and NIGHTINGALE M. P., Phys. Rev. Lett., 56 (1986) 742; AFFLECK I., Phys. Rev. Lett., 56 (1986) 746; MIRONOV A. D. and ZABRODIN A. V., Phys. Rev. Lett., 66 (1991) 534.
-
(1986)
Phys. Rev. Lett.
, vol.56
, pp. 746
-
-
Affleck, I.1
-
39
-
-
4244134837
-
-
CARDY J. L., Nucl. Phys. B, 270 (1986) 186; BLÖTE H. W. J., CARDY J. L. and NIGHTINGALE M. P., Phys. Rev. Lett., 56 (1986) 742; AFFLECK I., Phys. Rev. Lett., 56 (1986) 746; MIRONOV A. D. and ZABRODIN A. V., Phys. Rev. Lett., 66 (1991) 534.
-
(1991)
Phys. Rev. Lett.
, vol.66
, pp. 534
-
-
Mironov, A.D.1
Zabrodin, A.V.2
-
40
-
-
0007336674
-
-
note
-
The generalized random-phase-approximation for the spin-susceptibility is obtained by including ladder diagram vertex corrections to the single-loop susceptibility calculated with HF Greens functions.
-
-
-
-
41
-
-
0001062766
-
-
STERN F., Phys. Rev. Lett., 30 (1973) 278; ISIHARA A., Solid State Phys., 42 (1989) 271.
-
(1973)
Phys. Rev. Lett.
, vol.30
, pp. 278
-
-
Stern, F.1
-
42
-
-
77956917263
-
-
STERN F., Phys. Rev. Lett., 30 (1973) 278; ISIHARA A., Solid State Phys., 42 (1989) 271.
-
(1989)
Solid State Phys.
, vol.42
, pp. 271
-
-
Isihara, A.1
|