37 research outputs found
Magnon Bose condensation in symmetry breaking magnetic field
Magnon Bose condensation (BC)in the symmetry breaking magnetic field is a
result of unusual form of the Zeeman energy, which has terms linear in the
spin-wave operators and terms mixing excitations differ in the Wave-vector of
the magnetic structure. The following examples are considered: simple
easy-plane tetragonal antiferromagnets (AF), frustrated AF family
where etc. and cubic magnets with the Dzyaloshinskii-Moriya
interaction ( etc.). In all cases the BC becomes important when the
magnetic field becomes comparable with the spin-wave gap. The theory is
illustrated by existing experimental results.Comment: Submitted to J. of Phys. Condens. Matter (Proceedings of
International Conference "Highly Frustrated Magnets", Osaka (Japan), August
2006). 8 pages, 5 figure
Chiral criticality in doped MnFeSi compounds
The critical spin fluctuations in doped compounds MnFeSi have
been studied by means of ac-susceptibility measurements, polarized neutron
small angle scattering and spin echo spectroscopy. It is shown that these
compounds undergo the transition from the paramagnetic to helimagnetic phase
through continuous, yet well distinguishable crossovers: (i) from paramagnetic
to partially chiral, (ii) from partially chiral to highly chiral fluctuating
state. The crossover points are identified on the basis of combined analysis of
the temperature dependence of ac-susceptibility and polarized SANS data. The
whole transition is marked by two inflection point of the temperature
dependence of ac-susceptibility: the upper one corresponds to the crossover to
partially chiral state at , where the inverse correlation length , the lower one corresponds to the transition to the spin helix
structure. The intermediate crossover to the highly chiral phase is observed at
the inflection point of the first derivative of ac-susceptibility, where
. The temperature crossovers to the highly chiral fluctuating
state is associated with the enhancing influence of the Dzyaloshinskii-Moria
interaction close to .Comment: 5 pages, 5 figures, 1 table, 13 cite
Structure of a Solvated Nickel(II) Complex of (\u3cem\u3eS\u3c/em\u3e)-2\u27-(\u3cem\u3eN\u3c/em\u3e-benzylprolyl)aminoacetophenone and (\u3cem\u3eR\u3c/em\u3e)-valine Schiff base, C\u3csub\u3e25\u3c/sub\u3eH\u3csub\u3e29\u3c/sub\u3eN\u3csub\u3e3\u3c/sub\u3eNiO\u3csub\u3e3\u3c/sub\u3e.1/2C\u3csub\u3e4\u3c/sub\u3eH\u3csub\u3e8\u3c/sub\u3eO. Conformational Calculation of Diastereomeric Complexes of (\u3cem\u3eR\u3c/em\u3e)-valine and (\u3cem\u3eS\u3c/em\u3e)-valine
Magneto-elastic interaction in cubic helimagnets with B20 structure
The magneto-elastic interaction in cubic helimagnets with B20 symmetry is
considered. It is shown that this interaction is responsible for negative
contribution to the square of the spin-wave gap which is alone has to
disrupt assumed helical structure. It is suggested that competition between
positive part of which stems from magnon-magnon interaction and
its negative magneto-elastic part leads to the quantum phase transition
observed at high pressure in and . This transition has to occur
when . For from rough estimations at ambient pressure both
parts and are comparable with the experimentally
observed gap. The magneto-elastic interaction is responsible also for 2\m k
modulation of the lattice where \m k is the helix wave-vector and
contribution to the magnetic anisotropy.
Experimental observation by -ray and neutron scattering the lattice
modulation allows determine the strength of anisotropic part of the
magneto-elastic interaction responsible for above phenomena and the lattice
helicity
An Electron Spin Resonance Selection Rule for Spin-Gapped Systems
The direct electron spin resonance (ESR) absorption between a singlet ground
state and the triplet excited states of spin gap systems is investigated. Such
an absorption, which is forbidden by the conservation of the total spin quantum
number in isotropic Hamiltonians, is allowed by the Dzyaloshinskii-Moriya
interaction. We show a selection rule in the presence of this interaction,
using the exact numerical diagonalization of the finite cluster of the
quasi-one-dimensional bond-alternating spin system. The selection rule is also
modified into a suitable form in order to interpret recent experimental results
on CuGeO and NaVO.Comment: 5 pages, Revtex, with 6 eps figures, to appear in J. Phys. Soc. Jpn.
Vol. 69 No. 11 (2000
Spin chirality induced by the Dzyaloshinskii-Moriya interaction and the polarized neutron scattering
We discuss the influence of the Dzyaloshinskii-Moriya (DM) interaction in the
Heizenberg spin chain model for the observables in the polarized neutron
scattering experiments. We show that different choices of the parameters of DM
interaction may leave the spectrum of the problem unchanged, while the
observable spin-spin correlation functions may differ qualitatively.
Particularly, for the uniform DM interaction one has the incommensurate
fluctuations and polarization-dependent neutron scattering in the paramagnetic
phase. We sketch the possible generalization of our treatment to higher
dimensions.Comment: 4 pages, REVTEX, no figures, references added, to appear in PR
Role of domain wall fluctuations in non-Fermi liquid behavior of metamagnets
We study resistivity temperature dependence of a three dimensional metamagnet
near the metamagnet phase transition point in the case when magnetic structure
tends to split into regions with high and low magnetization. We show that in
the case of weak pinning the spin relaxation time of domain wall is much larger
than that of the volume spin fluctuations. This opens a temperature range where
resistivity temperature dependence is determined by scattering of conducting
electrons by the domain wall fluctuations. We show that it leads to
quasi-linear low temperature dependence of resistivity
ΠΠΎΡΠΌΠΎΠ½Π°Π»ΡΠ½ΠΎ-ΠΈΠΌΠΌΡΠ½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΡΠ°ΡΡΡ ΠΈ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΠΏΠΈΡΠ°Π½ΠΈΡ Ρ Π»ΠΈΡ Ρ ΠΎΠΆΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ
Nourishment peculiarities of 120 patients aged from 41 years having excess body mass and obesity were investigated. Interre-lations with changed hormonal-immune status were assessed. Method of food taking rate developed in the Institute of Nourishment, RAMS, taking into account nourishing peculiarities of Russian population was used. Study results revealed, that patients had imbal-ance concerning main macro- and micronutrients: nourishment regimen was disturbed in 90% of cases, taking main part of energy value was shifted to the second half of a day, increased calorie content of nourishment, excess of monosaccharides in the setting of decreased physical activity were seen which plays the main role in the development and advancing obesity, increased level of leuco-cytes, of TNF-Ξ±, IFN-Ξ³, humoral immunity link imbalance, increased serum concentration of leptin and insulin which is closely cor-relates with excess body mass and nourishment peculiarities.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΠΏΠΈΡΠ°Π½ΠΈΡ 120 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π² Π²ΠΎΠ·ΡΠ°ΡΡΠ΅ ΠΎΡ 18 Π΄ΠΎ 41 Π³ΠΎΠ΄Π° Ρ ΠΈΠ·Π±ΡΡΠΊΠΎΠΌ ΠΌΠ°ΡΡΡ ΡΠ΅Π»Π° ΠΈ ΠΎΠΆΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ. ΠΡΠ΅Π½Π΅Π½Ρ Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·ΠΈ Ρ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡΠΌΠΈ Π³ΠΎΡΠΌΠΎΠ½Π°Π»ΡΠ½ΠΎ-ΠΈΠΌΠΌΡΠ½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΡΠ°ΡΡΡΠ°. ΠΡΠΈΠΌΠ΅Π½ΡΠ»ΡΡ ΠΌΠ΅ΡΠΎΠ΄ Π°Π½Π°Π»ΠΈΠ·Π° ΡΠ°ΡΡΠΎΡΡ ΠΏΠΎΡΡΠ΅Π±Π»Π΅Π½ΠΈΡ ΠΏΠΈΡΠΈ, ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΡΠΉ Π² ΠΠ½ΡΡΠΈΡΡΡΠ΅ ΠΏΠΈΡΠ°Π½ΠΈΡ Π ΠΠΠ Ρ ΡΡΠ΅ΡΠΎΠΌ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠ΅ΠΉ ΠΏΠΈΡΠ°Π½ΠΈΡ Π½Π°ΡΠ΅Π»Π΅Π½ΠΈΡ Π ΠΎΡΡΠΈΠΈ. ΠΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π½Π°Π±Π»ΡΠ΄Π°Π»ΡΡ Π΄ΠΈΡΠ±Π°Π»Π°Π½Ρ ΠΏΠΎ ΠΎΡΠ½ΠΎΠ²Π½ΡΠΌ ΠΌΠ°ΠΊΡΠΎ- ΠΈ ΠΌΠΈΠΊΡΠΎΠ½ΡΡΡΠΈΠ΅Π½ΡΠ°ΠΌ, ΠΏΡΠΈΠΌΠ΅ΡΠ½ΠΎ Π² 90% ΡΠ»ΡΡΠ°Π΅Π² Π½Π°ΡΡΡΠ΅Π½ ΡΠ΅ΠΆΠΈΠΌ ΠΏΠΈΡΠ°Π½ΠΈΡ, ΠΏΡΠΈΠ΅ΠΌ ΠΎΡΠ½ΠΎΠ²Π½ΠΎΠΉ ΡΠ°ΡΡΠΈ ΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅Π½Π½ΠΎΡΡΠΈ ΡΠ°ΡΠΈΠΎΠ½Π° ΡΠΌΠ΅ΡΠ΅Π½ Π½Π° Π²ΡΠΎΡΡΡ ΠΏΠΎΠ»ΠΎΠ²ΠΈΠ½Ρ Π΄Π½Ρ, ΠΎΡΠΌΠ΅ΡΠ΅Π½Ρ ΡΠΎΡΡ ΠΎΠ±ΡΠ΅ΠΉ ΠΊΠ°Π»ΠΎΡΠΈΠΉΠ½ΠΎΡΡΠΈ ΠΏΠΈΡΠ°Π½ΠΈΡ, ΠΈΠ·Π±ΡΡΠΎΠΊ ΠΌΠΎΠ½ΠΎΡΠ°Ρ
Π°ΡΠΈΠ΄ΠΎΠ², ΠΆΠΈΡΠΎΠ² Π½Π° ΡΠΎΠ½Π΅ ΠΏΡΠΎΠ³ΡΠ΅ΡΡΠΈΡΡΡΡΠ΅Π³ΠΎ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ, Π° Π·Π½Π°ΡΠΈΡ ΠΈ ΡΠ½Π΅ΡΠ³ΠΎΠ·Π°ΡΡΠ°Ρ, ΡΡΠΎ ΠΈΠ³ΡΠ°Π΅Ρ ΠΎΡΠ½ΠΎΠ²Π½ΡΡ ΡΠΎΠ»Ρ Π² ΡΠ°Π·Π²ΠΈΡΠΈΠΈ ΠΈ ΠΏΡΠΎΠ³ΡΠ΅ΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΎΠΆΠΈΡΠ΅Π½ΠΈΡ, ΠΎΡΠΌΠ΅ΡΠ°Π΅ΡΡΡ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΠ΅ ΡΡΠΎΠ²Π½Ρ Π»Π΅ΠΉΠΊΠΎΡΠΈΡΠΎΠ², TNF-Ξ±, IFN-Ξ³, Π΄ΠΈΡΠ±Π°Π»Π°Π½Ρ Π³ΡΠΌΠΎΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π·Π²Π΅Π½Π° ΠΈΠΌΠΌΡΠ½ΠΈΡΠ΅ΡΠ°, ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΠ΅ ΡΡΠ²ΠΎΡΠΎΡΠΎΡΠ½ΠΎΠΉ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ Π»Π΅ΠΏΡΠΈΠ½Π° ΠΈ ΠΈΠ½ΡΡΠ»ΠΈΠ½Π°, ΡΠ΅ΡΠ½ΠΎ ΠΊΠΎΡΡΠ΅Π»ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ΅ Ρ ΠΠΠ’ ΠΈ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΡΠΌΠΈ ΠΏΠΈΡΠ°Π½ΠΈΡ