160 research outputs found
Ground-State Phase Diagram of Frustrated Anisotropic Quantum Spin Chains
Recent studies on the frustrated quantum spin chains with easy-plane
anisotropy are reviewed. We are particularly interested in novel "chiral"
phases characterized by the spontaneous breaking of the parity symmetry. The
ground-state phase diagrams of the chains are discussed.Comment: 6 pages (ptptex.sty), 3 figures, to appear in Prog. Theor. Phys.
Suppl. (Proc. of the 16th Nishinomiya-Yukawa Symposium and YITP International
Workshop, Nov. 2001
NMR relaxation rate in the field-induced octupolar liquid phase of spin-1/2 J1-J2 frustrated chains
In the spin-1/2 frustrated chain with nearest-neighbor ferromagnetic exchange
J1 and next-nearest-neighbor antiferromagnetic exchange J2 under magnetic
field, magnetic multipolar-liquid (quadrupolar, octupolar, and hexadecapolar)
phases are widely expanded from the saturation down to a low-field regime.
Recently, we have clarified characteristic temperature and field dependence of
the NMR relaxation rate 1/T_1 in the quadrupolar phase. In this paper, we
examine those of 1/T_1 in the octupolar phase combining field theoretical
method with numerical data. The relevance of the results to quasi
one-dimensional J1-J2 magnets such as PbCuSO4(OH)2, Rb2Cu2Mo3O12 and Li2ZrCuO4
is shortly discussed.Comment: 6 pages (1 column), 3 figure
Structural Analysis and Control of a Model of Two-site Electricity and Heat Supply
This paper introduces a control problem of regulation of energy flows in a
two-site electricity and heat supply system, where two Combined Heat and Power
(CHP) plants are interconnected via electricity and heat flows. The control
problem is motivated by recent development of fast operation of CHP plants to
provide ancillary services of power system on the order of tens of seconds to
minutes. Due to the physical constraint that the responses of the heat
subsystem are not necessary as fast as those of the electric subsystem, the
target controlled state is not represented by any isolated equilibrium point,
implying that stability of the system is lost in the long-term sense on the
order of hours. In this paper, we first prove in the context of nonlinear
control theory that the state-space model of the two-site system is non-minimum
phase due to nonexistence of isolated equilibrium points of the associated zero
dynamics.Instead, we locate a one-dimensional invariant manifold that
represents the target controlled flows completely. Then, by utilizing a virtual
output under which the state-space model becomes minimum phase, we synthesize a
controller that achieves not only the regulation of energy flows in the
short-term regime but also stabilization of an equilibrium point in the
long-term regime. Effectiveness of the synthesized controller is established
with numerical simulations with a practical set of model parameters
Boundary contributions to specific heat and susceptibility in the spin-1/2 XXZ chain
Exact low-temperature asymptotic behavior of boundary contribution to
specific heat and susceptibility in the one-dimensional spin-1/2 XXZ model with
exchange anisotropy 1/2 < \Delta \le 1 is analytically obtained using the
Abelian bosonization method. The boundary spin susceptibility is divergent in
the low-temperature limit. This singular behavior is caused by the first-order
contribution of a bulk leading irrelevant operator to boundary free energy. The
result is confirmed by numerical simulations of finite-size systems. The
anomalous boundary contributions in the spin isotropic case are universal.Comment: 6 pages, 3 figures; corrected typo
Spin-Nematic and Spin-Density-Wave Orders in Spatially Anisotropic Frustrated Magnets in a Magnetic Field
We develop a microscopic theory of finite-temperature spin-nematic orderings
in three-dimensional spatially anisotropic magnets consisting of weakly-coupled
frustrated spin-1/2 chains with nearest-neighbor and next-nearest-neighbor
couplings in a magnetic field. Combining a field theoretical technique with
density-matrix renormalization group results, we complete finite-temperature
phase diagrams in a wide magnetic-field range that possess spin-bond-nematic
and incommensurate spin-density-wave ordered phases. The effects of a four-spin
interaction are also studied. The relevance of our results to
quasi-one-dimensional edge-shared cuprate magnets such as LiCuVO4 is discussed.Comment: 5 pages (2 column version), 4 figures, Revtex, published versio
Renormalization of impurity scattering in one-dimensional interacting electron systems in magnetic field
We study the renormalization of a single impurity potential in
one-dimensional interacting electron systems in the presence of magnetic field.
Using the bosonization technique and Bethe ansatz solutions, we determine the
renormalization group flow diagram for the amplitudes of scattering of up- and
down-spin electrons by the impurity in a quantum wire at low electron density
and in the Hubbard model at less than half filling. In the absence of magnetic
field the repulsive interactions are known to enhance backscattering and make
the impurity potential impenetrable in the low-energy limit. On the contrary,
we show that in a strong magnetic field the interaction may suppress the
backscattering of majority-spin electrons by the impurity potential in the
vicinity of the weak-potential fixed point. This implies that in a certain
temperature range the impurity becomes almost transparent for the majority-spin
electrons while it is impenetrable for the minority-spin ones. The impurity
potential can thus have a strong spin-filtering effect.Comment: 11 pages, 2 figures; v2: a typo corrected and a reference added; v3:
published version, Sec.II revised with an additional explanatory subsection,
comments on the case of more than half-filling added, typos corrected, a
reference update
Dilute-Bose-Gas Approach to ground state phases of 3D quantum helimagnets under high magnetic field
We study high-field phase diagram and low-energy excitations of
three-dimensional quantum helimagnets. Slightly below the saturation field, the
emergence of magnetic order may be mathematically viewed as Bose-Einstein
condensation (BEC) of magnons. The method of dilute Bose gas enables an
unbiased quantitative analysis of quantum effects in three-dimensional
helimagnets and thereby three phases are found: cone, coplanar fan and an
attraction-dominant one. To investigate the last phase, we extend the usual BEC
approach so that we can handle 2-magnon bound states. In the case of 2-magnon
BEC, the transverse magnetization vanishes and long-range order occurs in the
quadrupolar channel (spin-nematic phase). As an application, we map out the
phase diagram of a 3D helimagnet which consists of frustrated J1-J2 chains
coupled by an interchain interaction J3.Comment: 4pages, 3figures, International Conference on Magnetism (ICM) 2009
(Karlsruhe, Germany, July 26-31, 2009)
Field and temperature dependence of the NMR relaxation rate in the magnetic quadrupolar liquid phase of spin-1/2 frustrated ferromagnetic chains
It is generally difficult to experimentally distinguish magnetic multipolar
orders in spin systems. Recently, it was proposed that the temperature
dependence of the nuclear magnetic resonance relaxation rate 1/T_1 can involve
an indirect, but clear signature of the field-induced spin nematic or
multipolar Tomonaga-Luttinger (TL) liquid phase [Phys. Rev. B79, 060406(R)
(2009)]. In this paper, we evaluate accurately the field and temperature
dependence of 1/T_1 in spin-1/2 frustrated J1-J2 chains combining
field-theoretical techniques with numerical data. Our results demonstrate that
isotherms of 1/T_1 as a function of magnetic field also exhibit distinctive
non-monotonic behavior in spin nematic TL liquid, in contrast with the standard
TL liquid in the spin-1/2 Heisenberg chain. The relevance of our results to
quasi one-dimensional edge-sharing cuprate magnets, such as LiCuVO4, is
discussed.Comment: 11 pages (2 column), 5 figures, published versio
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