-
1
-
-
0031482045
-
-
S.L. Sondhi, S.M. Girvin, J.P. Carini, and D. Shahar, Rev. Mod. Phys. 69, 315 (1997).
-
(1997)
Rev. Mod. Phys.
, vol.69
, pp. 315
-
-
Sondhi, S.L.1
Girvin, S.M.2
Carini, J.P.3
Shahar, D.4
-
4
-
-
33744711426
-
-
World Scientific, Singapore, also see (unpublished)
-
J. Richter, S. E. Krüger, D. J. J. Farnell, and R. F. Bishop, in Series on Advances in Quantum Many-Body Theory (World Scientific, Singapore, 2001), Vol. 5, p. 239 [also see (unpublished)].
-
(2001)
Series on Advances in Quantum Many-Body Theory
, vol.5
, pp. 239
-
-
Richter, J.1
Krüger, S.E.2
Farnell, D.J.J.3
Bishop, R.F.4
-
9
-
-
0001312603
-
-
F. Iglói, L. Turban, D. Karevski, and F. Szalma, Phys. Rev. B 56, 11 031 (1997).
-
(1997)
Phys. Rev. B
, vol.56
, pp. 11 031
-
-
Iglói, F.1
Turban, L.2
Karevski, D.3
Szalma, F.4
-
10
-
-
0000268055
-
-
C. Pich, A.P. Young, H. Rieger, and N. Kawashima, Phys. Rev. Lett. 81, 5916 (1998).
-
(1998)
Phys. Rev. Lett.
, vol.81
, pp. 5916
-
-
Pich, C.1
Young, A.P.2
Rieger, H.3
Kawashima, N.4
-
18
-
-
85038312845
-
-
Note, that the critical condition found in Ref. 17 [Eq. (6) of that paper] in our notations reads (formula presented) and can yield only two critical fields. However, by symmetry arguments (i.e., performing simple rotations of spin axes) one concludes that in addition to that condition there is an excitation of zero energy when (formula presented) and thus either two or four critical fields may appear
-
Note, that the critical condition found in Ref. 17 [Eq. (6) of that paper] in our notations reads (formula presented) and can yield only two critical fields. However, by symmetry arguments (i.e., performing simple rotations of spin axes) one concludes that in addition to that condition there is an excitation of zero energy when (formula presented) and thus either two or four critical fields may appear.
-
-
-
-
19
-
-
85038266211
-
-
We may consider also a chain of period 2 with (formula presented) and examine the GS properties as I varies. Then we find that for small (formula presented) there are two values of (formula presented) at which the system becomes gapless, whereas for large (formula presented) there are four such values of (formula presented) In general, condition (3) may be tuned by some parameter(s) influencing the local fields or/and exchange interactions
-
We may consider also a chain of period 2 with (formula presented) and examine the GS properties as I varies. Then we find that for small (formula presented) there are two values of (formula presented) at which the system becomes gapless, whereas for large (formula presented) there are four such values of (formula presented) In general, condition (3) may be tuned by some parameter(s) influencing the local fields or/and exchange interactions.
-
-
-
|