1,780 research outputs found
Magnetic and Structural Studies of the Quasi-Two-Dimensional Spin-Gap System (CuCl)LaNb2O7
We report magnetization, nuclear magnetic resonance (NMR), nuclear quadrupole
resonance (NQR), and transmission electron microscopy (TEM) studies on the
quasi-two-dimensional spin-gap system (CuCl)LaNb2O7, a possible candidate for
the J1-J2 model on a square lattice. A sharp single NQR line is observed at the
Cu and Cl sites, indicating that both Cu and Cl atoms occupy a unique site.
However, the electric field gradient tensors at the Cu, Cl, and La sites do not
have axial symmetry. This is incompatible with the reported crystal structure.
Thus the J1-J2 model has to be modified. We propose alternative two-dimensional
dimer models based on the NMR, NQR, and TEM results. The value of the hyperfine
coupling constant at the Cu sites indicates that the spin density is mainly on
the d(3z2-r2) orbital (z parallel c). At 1.5 K, Cu- and Nb-NMR signals
disappear above the critical field Bc1 = 10.3 T determined from the onset of
the magnetization, indicating a field-induced magnetic phase transition at Bc1.Comment: 9 pages, 16 figure
Collective Singlet Excitations and Evolution of Raman Spectral Weights in the 2D Spin Dimer Compound SrCu2(BO3)2
We present a Raman light scattering study of the two-dimensional quantum spin
system SrCu2(BO3)2 and show that the magnetic excitation spectrum has a rich
structure, including several well-defined bound state modes at low temperature,
and a scattering continuum and quasielastic light scattering contributions at
high temperature. The key to the understanding of the unique features of
SrCu2(BO3)2 is the presence of strong interactions between well-localized
triplet excitations in the network of orthogonal spin dimers realized in this
compound. Based on our analysis of the Heisenberg model relevant for this
material, we argue that the collective excitations involving two and
three-particle singlet bound states have large binding energies and are
observed as well-defined peaks in the Raman spectrum.Comment: 5 pages, 2 figures. Revised version, to appear in Phys. Rev. Lett.
(2000
Strong damping of phononic heat current by magnetic excitations in SrCu_2(BO_3)_2
Measurements of the thermal conductivity as a function of temperature and
magnetic field in the 2D dimer spin system SrCu(BO) are presented.
In zero magnetic field the thermal conductivity along and perpendicular to the
magnetic planes shows a pronounced double-peak structure as a function of
temperature. The low-temperature maximum is drastically suppressed with
increasing magnetic field. Our quantitative analysis reveals that the heat
current is due to phonons and that the double-peak structure arises from
pronounced resonant scattering of phonons by magnetic excitations.Comment: a bit more than 4 pages, 2 figures included; minor changes to improve
the clarity of the presentatio
Geodynamo and mantle convection simulations on the Earth Simulator using the Yin-Yang grid
We have developed finite difference codes based on the Yin-Yang grid for the
geodynamo simulation and the mantle convection simulation. The Yin-Yang grid is
a kind of spherical overset grid that is composed of two identical component
grids. The intrinsic simplicity of the mesh configuration of the Yin-Yang grid
enables us to develop highly optimized simulation codes on massively parallel
supercomputers. The Yin-Yang geodynamo code has achieved 15.2 Tflops with 4096
processors on the Earth Simulator. This represents 46% of the theoretical peak
performance. The Yin-Yang mantle code has enabled us to carry out mantle
convection simulations in realistic regimes with a Rayleigh number of
including strongly temperature-dependent viscosity with spatial contrast up to
.Comment: Plenary talk at SciDAC 200
Promotive effects of hyperthermia on the Ρytostatic activity to ehrlich ascites tumor cells by diverse delta-alkyllactones
To evaluate promotive effects of hyperthermia on antitumor activity of new delta-alkyllactones (DALs) of low molecular weight (184β254 Da), chemically synthesized, which are different from natural macrocyclic lactones of high molecular weight (348β439 Da), such as camptothecin and sultriecin. Methods: A suspension of Ehrlich ascites tumor (EAT) cells was mixed with a DAL in a glass tube, heated at 37 or 42 Β°C for 30 min in a water bath, and cultured at 37 Β°C for 20 or 72 h. Cell viability was measured by the mitochondrial dehydrogenase- based WST-1 assay. DALs incorporated into EAT cells was extracted and measured by gas-liquid chromatography. Results: The reduction of cell viability by DALs was markedly enhanced upon the treatment at 42 Β°C compared to that at 37 oC. At 37 oC, delta-hexadecalactone (DH16 : 0) and delta-tetradecalactone (DTe14 : 0) displayed cytostatic activity (at 100 Β΅M survival level: 20.7%, 66.1%; at 50 Β΅M β 41.2%, 82.4%, respectively). Their activity was more marked at 42 Β°C (at 100 Β΅M 10.6%, 27.6%; at 50 Β΅M 30.6, 37.5 %, ibid). The other DALs, delta-undecalactone (DU11 : 0), delta-dodecalactone (DD12 : 0), and delta-tridecanolactone (DTr13 : 0) were almost ineffective. Evaluation of survival rate in the cells treated for 30 min by DALs with the next culturing of EAT cells for 72 h resulted in the enhanced carcinostatic activity of DH16:0 and DTe14:0 even at concentrations as low as 25 Β΅M at either 37 Β°C (18.5%, 78.5%, ibid) or 42 Β°C (5.0%, 42.0%, ibid), but the others exhibited slight activity or none. DH16 : 0 was effective at either 37 Β°C (36.0%) or 42 Β°C (23.0%) even at a lower dose of 10 Β΅M. At the same time only the most cytostatic DH16 : 0 was incorporated into EAT cells and the rate of incorporation was more at 42 Β°C than at 37 Β°C. Conclusion: Delta-hexadecanolactone (DH16 : 0) exhibited the most cytostatic effect that was significantly enhanced by hyperthermia. It allows to consider it as a potent antitumor agent, especially in combination with hyperthermia.Π¦Π΅Π»Ρ: ΠΎΡΠ΅Π½ΠΈΡΡ ΠΏΡΠΎΠΌΠΎΡΠΎΡΠ½ΡΠΉ ΡΡΡΠ΅ΠΊΡ Π³ΠΈΠΏΠ΅ΡΡΠ΅ΡΠΌΠΈΠΈ Π½Π° ΠΏΡΠΎΡΠΈΠ²ΠΎΠΎΠΏΡΡ
ΠΎΠ»Π΅Π²ΡΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ Π½ΠΎΠ²ΡΡ
Π½ΠΈΠ·ΠΊΠΎΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΡ
(184β254 ΠΠ°)
Π΄Π΅Π»ΡΡΠ°-Π°Π»ΠΊΠΈΠ»Π»Π°ΠΊΡΠΎΠ½ΠΎΠ² (DALs), Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈ ΡΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΈΠ· ΡΠ°Π·Π½ΡΡ
ΠΌΠ°ΠΊΡΠΎΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΡΡΠΎΠΊΠΎΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΡ
(348β439ΠΠ°)
Π»Π°ΠΊΡΠΎΠ½ΠΎΠ² Π΅ΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΠΏΡΠΎΠΈΡΡ
ΠΎΠΆΠ΄Π΅Π½ΠΈΡ, ΡΠ°ΠΊΠΈΡ
ΠΊΠ°ΠΊ ΠΊΠ°ΠΌΠΏΡΠΎΡΠ΅ΡΠΈΠ½ ΠΈ ΡΠ°Π»ΡΡΠΈΠ΅ΡΠΈΠ½. ΠΠ΅ΡΠΎΠ΄Ρ: ΡΡΡΠΏΠ΅Π½Π·ΠΈΡ ΠΊΠ»Π΅ΡΠΎΠΊ Π°ΡΡΠΈΡΠ½ΠΎΠΉ ΠΎΠΏΡΡ
ΠΎΠ»ΠΈ
ΠΡΠ»ΠΈΡ
Π° (EAT) ΡΠΌΠ΅ΡΠΈΠ²Π°Π»ΠΈ Ρ DAL Π² ΡΡΠ΅ΠΊΠ»ΡΠ½Π½ΠΎΠΉ ΠΏΡΠΎΠ±ΠΈΡΠΊΠ΅, Π½Π°Π³ΡΠ΅Π²Π°Π»ΠΈ Π΄ΠΎ 37 Β°C ΠΈΠ»ΠΈ 42 Β°C Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ 30 ΠΌΠΈΠ½ Π½Π° Π²ΠΎΠ΄ΡΠ½ΠΎΠΉ Π±Π°Π½Π΅
ΠΈ Π΄Π°Π»Π΅Π΅ ΠΊΡΠ»ΡΡΠΈΠ²ΠΈΡΠΎΠ²Π°Π»ΠΈ ΠΏΡΠΈ 37 Β°C Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ 20 ΠΈΠ»ΠΈ 72 Ρ. ΠΡΠ΅Π½ΠΊΡ ΠΆΠΈΠ·Π½Π΅ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΠΈ ΠΊΠ»Π΅ΡΠΎΠΊ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ WST-1
Π°Π½Π°Π»ΠΈΠ·Π°, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ Π½Π° ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠΈ ΠΌΠΈΡΠΎΡ
ΠΎΠ½Π΄ΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ Π΄Π΅Π³ΠΈΠ΄ΡΠΎΠ³Π΅Π½Π°Π·Ρ. ΠΠ½ΠΊΠΎΡΠΏΠΎΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠ΅ Π² EAT-ΠΊΠ»Π΅ΡΠΊΠΈ DALs ΡΠΊΡΡΡΠ°Π³ΠΈΡΠΎΠ²Π°Π»ΠΈ,
ΠΈΡ
ΡΡΠΎΠ²Π΅Π½Ρ ΠΈΠ·ΠΌΠ΅ΡΡΠ»ΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ Π³Π°Π·ΠΎ-ΠΆΠΈΠ΄ΠΊΠΎΡΡΠ½ΠΎΠΉ Ρ
ΡΠΎΠΌΠ°ΡΠΎΠ³ΡΠ°ΡΠΈΠΈ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ: DALs Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΡΠ½ΠΈΠΆΠ°Π»ΠΈ
ΠΆΠΈΠ·Π½Π΅ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΡ ΠΊΠ»Π΅ΡΠΎΠΊ ΠΏΠΎΡΠ»Π΅ ΠΏΡΠ΅Π΄Π²Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ ΠΏΡΠΈ 42 Β°C ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ 37 Β°C. ΠΡΠΈ 37 Β°C Π±ΡΠ»ΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΌΠΈ
Π΄Π΅Π»ΡΡΠ°-Π³Π΅ΠΊΡΠ°Π΄Π΅ΠΊΠ°Π»Π°ΠΊΡΠΎΠ½ (DH16 : 0) ΠΈ Π΄Π΅Π»ΡΡΠ°-ΡΠ΅ΡΡΠ°Π΄Π΅ΠΊΠ°Π»Π°ΠΊΡΠΎΠ½ (DTe14 : 0) (ΠΏΡΠΈ 100 ΞΌM ΡΡΠΎΠ²Π΅Π½Ρ Π²ΡΠΆΠΈΠ²Π°Π΅ΠΌΠΎΡΡΠΈ: 20,7; 66,1%;
ΠΏΡΠΈ 50 ΞΌM β 41,2; 82,4% ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²Π΅Π½Π½ΠΎ). ΠΡΠΎΡ ΡΡΡΠ΅ΠΊΡ Π±ΡΠ» Π±ΠΎΠ»Π΅Π΅ Π²ΡΡΠ°ΠΆΠ΅Π½Π½ΡΠΌ ΠΏΡΠΈ 42 Β°C (ΠΏΡΠΈ 100 ΞΌM 10,6; 27,6%; ΠΏΡΠΈ
50ΞΌM 30,6; 37,5% ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²Π΅Π½Π½ΠΎ). ΠΡΡΠ³ΠΈΠ΅ DALs, Π° ΠΈΠΌΠ΅Π½Π½ΠΎ Π΄Π΅Π»ΡΡΠ°-ΡΠ½Π΄Π΅ΠΊΠ°Π»Π°ΠΊΡΠΎΠ½ (DU11 : 0), Π΄Π΅Π»ΡΡΠ°-Π΄ΠΎΠ΄Π΅ΠΊΠ°Π»Π°ΠΊΡΠΎΠ½ (DD12 : 0)
ΠΈ Π΄Π΅Π»ΡΡΠ°-ΡΡΠΈΠ΄Π΅ΠΊΠ°Π»Π°ΠΊΡΠΎΠ½ (DTr13 : 0) Π±ΡΠ»ΠΈ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½Ρ. ΠΡΠ΅Π½ΠΊΠ° ΡΡΠΎΠ²Π½Ρ Π²ΡΠΆΠΈΠ²Π°Π΅ΠΌΠΎΡΡΠΈ EAT-ΠΊΠ»Π΅ΡΠΎΠΊ, 30 ΠΌΠΈΠ½
ΠΎΠ±ΡΠ°Π±ΠΎΡΠ°Π½Π½ΡΡ
DALs Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠΈΠΌ ΠΊΡΠ»ΡΡΠΈΠ²ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ 72 Ρ, ΠΏΠΎΠΊΠ°Π·Π°Π»Π° ΠΏΠΎΠ²ΡΡΠ΅Π½Π½ΡΡ ΠΊΠ°Π½ΡΠ΅ΡΠΎΡΡΠ°ΡΠΈΡΡΠ΅ΠΊΡΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ
DH16 : 0 ΠΈ DTe14 :0 Π΄Π°ΠΆΠ΅ ΠΏΡΠΈ 25 ΞΌM ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ, ΠΊΠ°ΠΊ ΠΏΡΠΈ 37 Β°C (18,5; 78,5% ΡΠΎΠΎΡΠ²Π΅ΡΡΠ²Π΅Π½Π½ΠΎ), ΡΠ°ΠΊ ΠΈ ΠΏΡΠΈ 42 Β°C (5,0; 42,0%
ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²Π΅Π½Π½ΠΎ). ΠΠ»Ρ Π΄ΡΡΠ³ΠΈΡ
DALs Π΄Π°Π½Π½ΡΠΉ ΡΡΡΠ΅ΠΊΡ Π±ΡΠ» Π½Π΅Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΠΉ Π»ΠΈΠ±ΠΎ ΠΎΡΡΡΡΡΡΠ²ΠΎΠ²Π°Π». DH16 : 0 ΠΎΡΡΠ°Π²Π°Π»ΡΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΌ
ΠΊΠ°ΠΊ ΠΏΡΠΈ 37 Β°C (36,0%), ΡΠ°ΠΊ ΠΈ ΠΏΡΠΈ 42 Β°C (23,0%) Π² 10 ΞΌM ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ. Π ΡΠΎ ΠΆΠ΅ Π²ΡΠ΅ΠΌΡ ΡΠΎΠ»ΡΠΊΠΎ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΉ
DAL β DH16 : 0 ΠΈΠ½ΠΊΠΎΡΠΏΠΎΡΠΈΡΠΎΠ²Π°Π»ΡΡ Π² ΠΊΠ»Π΅ΡΠΊΠΈ EAT, ΠΈ ΡΡΠΎΠ²Π΅Π½Ρ ΠΈΠ½ΠΊΠΎΡΠΏΠΎΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π±ΡΠ» Π²ΡΡΠ΅ ΠΏΡΠΈ 42 Β°C, ΡΠ΅ΠΌ ΠΏΡΠΈ 37 Β°C. ΠΡΠ²ΠΎΠ΄Ρ:
Π΄Π΅Π»ΡΡΠ°-Π³Π΅ΠΊΡΠ°Π΄Π΅ΠΊΠ°Π½ΠΎΠ»Π°ΠΊΡΠΎΠ½ (DH16 : 0) ΠΏΠΎΠΊΠ°Π·Π°Π» Π½Π°ΠΈΠ±ΠΎΠ»ΡΡΡΡ ΡΠΈΡΠΎΡΡΠ°ΡΠΈΡΠ΅ΡΠΊΡΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ, ΠΊΠΎΡΠΎΡΠ°Ρ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΡΡΠΈΠ»ΠΈΠ²Π°Π»Π°ΡΡ
Π² ΠΊΠΎΠΌΠ±ΠΈΠ½Π°ΡΠΈΠΈ Ρ Π³ΠΈΠΏΠ΅ΡΡΠ΅ΡΠΌΠΈΠ΅ΠΉ. ΠΡΠΎΡ DAL ΠΌΠΎΠΆΠ½ΠΎ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°ΡΡ ΠΊΠ°ΠΊ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΠΉ ΡΠΈΡΠΎΡΡΠ°ΡΠΈΠΊ, Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ ΡΡΠΈΠ»ΠΈΠ²Π°Π΅ΡΡΡ
ΠΏΡΠΈ Π³ΠΈΠΏΠ΅ΡΡΠ΅ΡΠΌΠΈΠΈ
BiCuVO: a new narrow-band spin-gap material
A new spin-ladder family material BiCuVO is studied by means of the
magnetic susceptibility, heat capacity and neutron inelastic scattering
measurements on powder sample. Singlet ground state and a finite spin gap are
confirmed by thermal-activated type susceptibility and by distinct peak at 16
meV in spin excitation. Triple narrow band structure in spin excitation
spectrum, probably due to complex crystal structure, is observed and the
possibility of weakly-interacting spin-cluster system is discussed
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