-
4
-
-
85038311381
-
-
Formally, a language is defined by a set of operators each acting irreducibly on a local Hilbert space of dimension D. The language does not determine the quantum dynamics of the system (which is determined by the Hamiltonian) but the dynamics can be expressed in different languages. See Ref. 6
-
Formally, a language is defined by a set of operators each acting irreducibly on a local Hilbert space of dimension D. The language does not determine the quantum dynamics of the system (which is determined by the Hamiltonian) but the dynamics can be expressed in different languages. See Ref. 6.
-
-
-
-
6
-
-
85038307418
-
-
G. Ortiz and C.D. Batista, in Recent Progress in Many-Body Theories, edited by R.F. Bishop, T. Brandes, K.A. Gerhoth, N.R. Walet, and Y. Xian (World Scientific, Singapore, 2002), p. 425;
-
G. Ortiz and C.D. Batista, in Recent Progress in Many-Body Theories, edited by R.F. Bishop, T. Brandes, K.A. Gerhoth, N.R. Walet, and Y. Xian (World Scientific, Singapore, 2002), p. 425;
-
-
-
-
7
-
-
85038347294
-
-
cond-mat/0207076 (unpublished)
-
G. Ortiz and C.D. Batista, cond-mat/0207076 (unpublished).
-
-
-
Ortiz, G.1
Batista, C.D.2
-
8
-
-
85038265810
-
-
A. Auerbach, Interacting Electrons and Quantum Magnetism (Springer-Verlag, New York, 1994)
-
A. Auerbach, Interacting Electrons and Quantum Magnetism (Springer-Verlag, New York, 1994).
-
-
-
-
9
-
-
85038281891
-
-
cond-mat/0207106 (unpublished)
-
C.D. Batista and G. Ortiz, cond-mat/0207106 (unpublished).
-
-
-
Batista, C.D.1
Ortiz, G.2
-
10
-
-
85038271539
-
-
In the present manuscript the irrelevant constant terms in the transformed Hamiltonian operators are always omitted
-
In the present manuscript the irrelevant constant terms in the transformed Hamiltonian operators are always omitted.
-
-
-
-
12
-
-
85038271292
-
-
We know that for (Formula presented) we can find the exact ground and lowest-energy states of H.5
-
We know that for (Formula presented) we can find the exact ground and lowest-energy states of H.5
-
-
-
-
13
-
-
85038295261
-
-
One can add temporal fluctuations through a similar type of dynamical mean field as described in Ref. 13 but in the HL
-
One can add temporal fluctuations through a similar type of dynamical mean field as described in Ref. 13 but in the HL.
-
-
-
-
15
-
-
85038281837
-
-
If we are looking for solutions which could break the lattice translational symmetry (inhomogeneous), we should consider OP’s (Formula presented) for all possible (Formula presented) vectors. In general, nonlocal OP’s can be derived (starting from our local classification) similarly to what has been done in the literature. For instance, for a quantum (Formula presented) system there are two possible local OP’s: the local magnetization and the local spin-nematic parameters. Therefore, in the case of a quantum spin (Formula presented) glass there will be two types of glasses: One where the local magnetization is frozen at each site and another where the local spin-nematic order is frozen at each site. In other words, there will be two Edwards-Anderson OP’s
-
If we are looking for solutions which could break the lattice translational symmetry (inhomogeneous), we should consider OP’s (Formula presented) for all possible (Formula presented) vectors. In general, nonlocal OP’s can be derived (starting from our local classification) similarly to what has been done in the literature. For instance, for a quantum (Formula presented) system there are two possible local OP’s: the local magnetization and the local spin-nematic parameters. Therefore, in the case of a quantum spin (Formula presented) glass there will be two types of glasses: One where the local magnetization is frozen at each site and another where the local spin-nematic order is frozen at each site. In other words, there will be two Edwards-Anderson OP’s.
-
-
-
-
17
-
-
85038266174
-
-
Find a matrix (Formula presented) such that (Formula presented) and T satisfies the paraunitarity condition (Formula presented) with (Formula presented)The necessary and sufficient condition for an Hermitian matrix to be paraunitarily diagonalized (with all diagonal elements positive) is that the matrix be positive definite
-
Find a matrix (Formula presented) such that (Formula presented) and T satisfies the paraunitarity condition (Formula presented) with (Formula presented)The necessary and sufficient condition for an Hermitian matrix to be paraunitarily diagonalized (with all diagonal elements positive) is that the matrix be positive definite.
-
-
-
-
18
-
-
85038278199
-
-
In this case the eigenvalues can be determined in closed analytic form (Formula presented) (Formula presented) (Formula presented) (Formula presented) (Formula presented)
-
In this case the eigenvalues can be determined in closed analytic form (Formula presented) (Formula presented) (Formula presented) (Formula presented) (Formula presented)
-
-
-
-
19
-
-
85038317850
-
-
In two space dimensions, (Formula presented) (Formula presented) (Formula presented) and (Formula presented)
-
In two space dimensions, (Formula presented) (Formula presented) (Formula presented) and (Formula presented)
-
-
-
-
20
-
-
4243979698
-
-
A.E. Trumper, L.O. Manuel, C.J. Gazza, and H.A. Ceccatto, Phys. Rev. Lett. 78, 2216 (1997).
-
(1997)
Phys. Rev. Lett.
, vol.78
, pp. 2216
-
-
Trumper, A.E.1
Manuel, L.O.2
Gazza, C.J.3
Ceccatto, H.A.4
-
22
-
-
84870468859
-
-
X.-G. Wen, Phys. Rev. B. 65, 165113 (2002)
-
X.-G. Wen, Phys. Rev. B. 65, 165113 (2002).
-
-
-
|