259 research outputs found
First evidence for charge ordering in NaVO from Raman spectroscopy
We argue on the basis of symmetry selection rules and Raman scattering
spectra that NaVO undergoes a charge ordering phase transition at
T=34 K. Such a transition is characterized by the redistribution of the
charges at the phase transition and corresponds to the change of the vanadium
ions, from uniform V to two different V and V states. In
the low temperature phase the V ions are forming a "zig-zag" ladder
structure along the {\bf b}-axis, consistent with the symmetry of the P2/b
space group.Comment: to be published in solid state communication
Hybrid heterostructures with superconducting/antiferromagnetic interfaces
We report on structural, DC, X-ray and neutron studies of hybrid
superconducting mesa-heterostructures with a cuprate antiferromagnetic
interlayer Ca1-xSrxCuO2 (CSCO). The upper electrode was bilayer Nb/Au
superconductor and copper oxide superconductor YBa2Cu3O7 (YBCO) was the bottom
electrode. It was experimentally shown that during the epitaxial growth of the
two films YBCO and CSCO a charge carrier doping takes place in the CSCO
interlayer with a depth about 20 nm. The conductivity of the doped part of CSCO
layer is close to the metal type, while the reference CSCO film, deposited
directly on NdGaO3 substrate, behaves as Mott insulator with the hopping
conductivity. The interface Au/CSCO is clearly seen on bright-field image of
the cross-section of heterostructure and gives the main contribution to the
total resistance of mesa-heterostructure.Comment: 16 pages, 9 figure
Anomalous thermal conductivity of NaV2O5 as compared to conventional spin-Peierls system CuGeO3
A huge increase of thermal conductivity k is observed at the phase transition
in stoichiometric NaV2O5. This anomaly decreases and gradually disappears with
deviation from stoichiometry in Na(1-x}V2O5 (x = 0.01, 0.02, 0.03, and 0.04).
This behavior is compared with that of pure and Zn-doped CuGeO3 where only
modest kinks in the k(T) curves are observed at the spin-Peierls transition.
The change of k at critical temperature Tc could be partially attributed to the
opening of an energy gap in the magnetic excitation spectrum excluding the
scattering of thermal phonons on spin fluctuations. However, the reason for
such a strong anomaly in the k(T) may lie not only in the different energy
scales of CuGeO3 and NaV2O5, but also in the different character of the phase
transition in NaV2O5 which can have largely a structural origin, e.g. connected
with the charge ordering.Comment: PostScript 4 pages, 4 PostScript pictures. Submitted to Physical
Review Letter
Relationships of nosological form of the primary and second neoplasms in oncological patients
ΠΠΠΠΠΠ§ΠΠ‘Π’ΠΠΠΠΠ«Π ΠΠΠΠΠΠΠ ΠΠΠΠΠΠΠΠ―ΠΠΠΠΠΠΠΠΠ§ΠΠ‘ΠΠΠ Π€ΠΠ ΠΠ« Π ΠΠΠΠΠΠΠΠΠΠΠΠΠΠΠ‘Π’Π¬, Π§ΠΠ‘Π’ΠΠ’Π Π‘ΠΠ£Π§ΠΠΠΠ£ΠΠ ΠΠΠΠΠ¦Π΅Π»Ρ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΌΠ΅ΠΆΠ΄Ρ Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠΎΡΠΌΠ°ΠΌΠΈ ΠΏΠ΅ΡΠ²ΡΡ
ΠΈ Π²ΡΠΎΡΡΡ
ΡΠ°ΠΊΠΎΠ² Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΊΠΎΡΠΎΡΡΠ΅ ΠΏΡΠΎΡ
ΠΎΠ΄ΠΈΠ»ΠΈ ΡΠΏΠ΅ΡΠΈΠ°Π»ΡΠ½ΠΎΠ΅ Π»Π΅ΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρ ΠΎΠ½ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΡ ΠΈ Ρ ΠΊΠΎΡΠΎΡΡΡ
Π²ΠΎΠ·Π½ΠΈΠΊΠ»ΠΈ Π²ΡΠΎΡΡΠ΅ ΡΠ°ΠΊΠΈ ΡΠ΅ΡΠ΅Π· 3 Π³ΠΎΠ΄Π° ΠΈ Π±ΠΎΠ»Π΅Π΅ ΠΏΠΎΡΠ»Π΅ ΠΎΠΊΠΎΠ½ΡΠ°Π½ΠΈΡ Π»Π΅ΡΠ΅Π½ΠΈΡ. ΠΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. Π ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΎΡΡ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ ΠΌΠ΅ΠΆΠ΄Ρ Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΡΠΊΡΡΡΠΎΠΉ Π²ΡΠΎΡΡΡ
ΡΠ°ΠΊΠΎΠ², ΠΊΠΎΡΠΎΡΡΠ΅ Π²ΠΎΠ·Π½ΠΈΠΊΠ»ΠΈ Ρ 203 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΏΡΠΎΡ
ΠΎΠ΄ΠΈΠ²ΡΠΈΡ
Π»Π΅ΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρ ΠΎΠ½ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠΈ, ΠΈ ΠΎΡΠΈΡΠΈΠ°Π»ΡΠ½ΡΠΌΠΈ Π΄Π°Π½Π½ΡΠΌΠΈ ΠΎΠ± ΡΠ΄Π΅Π»ΡΠ½ΠΎΠΌ Π²Π΅ΡΠ΅ 10 ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΡΠΌ Π·Π»ΠΎΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
Π½ΠΎΠ²ΠΎΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠΉ Π½Π°ΡΠ΅Π»Π΅Π½ΠΈΡ Π£ΠΊΡΠ°ΠΈΠ½Ρ. Π‘ΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠ°Ρ Π·Π½Π°ΡΠΈΠΌΠΎΡΡΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΎΡΠ΅Π½ΠΈΠ²Π°Π»Π°ΡΡ Ρ ΠΏΠΎΠΌΠΎΡΡΡ Π΄ΠΎΠ²Π΅ΡΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»ΠΎΠ², Π½ΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Ρ ΡΡΠ΅ΡΠΎΠΌ ΡΠΏΠ΅ΡΠΈΡΠΈΠΊΠΈ ΠΊΠΎΠ½ΡΠΈΠ½Π³Π΅Π½ΡΠ° ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ, Π³Π΄Π΅ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΎΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. Π ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΈΠΈ Ρ ΡΠ΄Π΅Π»ΡΠ½ΡΠΌ Π²Π΅ΡΠΎΠΌ Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΡΠΌ ΠΏΠ΅ΡΠ²ΡΡ
ΡΠ°ΠΊΠΎΠ², ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»Π΅Π½Π½ΡΡ
, Π² ΠΏΠ΅ΡΠ²ΡΡ ΠΎΡΠ΅ΡΠ΅Π΄Ρ, ΡΠΏΠ΅ΡΠΈΠ°Π»ΠΈΠ·Π°ΡΠΈΠ΅ΠΉ ΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ, ΠΎΠ±ΡΠ»Π΅Π΄ΡΠ΅ΠΌΡΠ΅ Π³ΡΡΠΏΠΏΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π±ΡΠ»ΠΈ ΡΠ°Π·Π΄Π΅Π»Π΅Π½Ρ Π½Π° 5 Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ΄Π³ΡΡΠΏΠΏ: ΠΏΠ°ΡΠΈΠ΅Π½ΡΡ Ρ ΡΠ°ΠΊΠΎΠΌ ΠΌΠΎΠ»ΠΎΡΠ½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ, ΡΠΈΡΠΎΠ²ΠΈΠ΄Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ, ΡΠ΅Π»Π° ΠΌΠ°ΡΠΊΠΈ, ΡΠ΅ΠΉΠΊΠΈ ΠΌΠ°ΡΠΊΠΈ, ΡΠ°ΠΊ ΡΠΈΡΠ½ΠΈΠΊΠΎΠ² ΠΈ Ρ ΠΈΠ½ΡΠΌΠΈ ΡΠΎΡΠΌΠ°ΠΌΠΈ ΡΠ°ΠΊΠ°. ΠΠ»Ρ ΠΊΠ°ΠΆΠ΄ΠΎΠΉ ΠΈΠ· ΠΏΠΎΠ΄Π³ΡΡΠΏΠΏ Π±ΡΠ»Π° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π° Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΡΡΡΠΊΡΡΡΠ° Π²ΡΠΎΡΡΡ
ΡΠ°ΠΊΠΎΠ² ΠΈ ΡΠΎΠΏΠΎΡΡΠ°Π²Π»Π΅Π½Π° Ρ ΠΎΠ±ΡΠ΅ΠΉ ΡΡΡΡΠΊΡΡΡΠΎΠΉ Π·Π»ΠΎΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
Π½ΠΎΠ²ΠΎΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΠΎ Π΄Π°Π½Π½ΡΠΌ ΠΎΡΠΈΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ ΡΡΠ°ΡΠΈΡΡΠΈΠΊΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΠ°ΡΡΠΎΡΠ° ΠΏΡΡΠΈ Π²ΡΠ΄Π΅Π»Π΅Π½Π½ΡΡ
Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΡΠΌ, ΡΠ°ΡΡΡΠΈΡΠ°Π½Π½ΡΡ
Π΄Π»Ρ ΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ, Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎ Ρ
ΠΎΡΠΎΡΠΎ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΠ΅Ρ ΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΎΠ½Π½ΠΎΠΌΡ ΡΡΠ΅Π΄Π½Π΅ΠΌΡ, ΠΏΡΠΈ ΡΡΠΎΠΌ Π΄Π»Ρ Π΄Π²ΡΡ
Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²ΠΈΡΠ΅Π»ΡΠ½ΡΡ
Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΡΠΌ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΈΠ΅ Π½Π°Ρ
ΠΎΠ΄ΠΈΡΡΡ Π² ΠΏΡΠ΅Π΄Π΅Π»Π°Ρ
ΠΎΠΆΠΈΠ΄Π°Π΅ΠΌΠΎΠΉ ΡΡΠΎΡ
Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈΠ·ΠΌΠ΅Π½ΡΠΈΠ²ΠΎΡΡΠΈ. Π’Π°ΠΊΠΈΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ, ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Π½Π΅ ΡΡΡΠ΅ΡΡΠ²ΡΠ΅Ρ ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈ Π·Π½Π°ΡΠΈΠΌΡΡ
ΡΠ°Π·Π»ΠΈΡΠΈΠΉ ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΡΠΎΡΠ΅Π½ΡΠ½ΡΠΌ ΡΠΎΡΡΠ°Π²ΠΎΠΌ 10 ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΡΠΌ ΡΠ°ΠΊΠ° Π½Π°ΡΠ΅Π»Π΅Π½ΠΈΡ Π£ΠΊΡΠ°ΠΈΠ½Ρ ΠΈ ΡΡΡΡΠΊΡΡΡΠΎΠΉ Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΡΠΌ Π²ΡΠΎΡΡΡ
ΡΠ°ΠΊΠΎΠ² Ρ ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΠΎΠΉ Π³ΡΡΠΏΠΏΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ². ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΠΎΡΠΌΠ° Π²ΡΠΎΡΡΡ
ΡΠ°ΠΊΠΎΠ² Π½Π΅ ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠ΅ΠΌ ΠΏΠ΅ΡΠ²ΠΎΠ³ΠΎ ΡΠ°ΠΊΠ°, Π° Π²ΠΎΡΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΡ ΠΎΠ±ΡΡΡ Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΡΡ ΡΡΡΡΠΊΡΡΡΡ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π΅ΠΌΠΎΡΡΠΈ Π·Π»ΠΎΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΠΌΠΈ Π½ΠΎΠ²ΠΎΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡΠΌΠΈ.Objective. To investigate the relationship between nosological forms of the primary and second neoplasms in patients who have undergone special treatment for cancer, and who have developed second neoplasms three and more years after the end of treatment. Methods. The study has compared the nosological structure of second neoplasms that developed in 203 patients undergoing treatment for oncological pathology with the official data on the specific weight of 10 major nosological forms of malignant neoplasms in Ukraine. The statistical significance of the obtained results has been estimated using confidence intervals normalized taking into account the specificity of the patients of the clinic where the study was conducted. Results. In accordance with the specific weight of the nosological forms of the primary neoplasms, conditioned first by the specialization of the clinic, the study groups were divided into 5 nosological subgroups: patients with breast, thyroid, uterine, cervical, ovarian, and subgroup with other forms of cancer. For each of the subgroups, the nosological structure of the second neoplasms was investigated and compared with the overall structure of malignant neoplasms according to the official statistics. It is shown that the frequencies of five allocated nosological forms calculated for the clinic correspond fairly well to the population mean, while for two most representative nosological forms the correspondence is within the expected stochastic variability. Thus, it has been demonstrated that there are no statistically significant differences between the percentage composition of 10 major nosological forms of cancer in Ukraine and the structure of nosological forms of second neoplasms in the study group of patients. Conclusions. The nosological form of second neoplasms is not a consequence of the primary cancer, but reproduces the overall nosological structure of the incidence of malignant neoplasms
Enhancement of the Thermal Conductivity in gapped Quantum Spin Chains
We study mechanism of magnetic energy transport, motivated by recent
measurements of the thermal conductivity in low dimensional quantum magnets. We
point out a possible mechanism of enhancement of the thermal conductivity in
gapped magnetic system, where the magnetic energy transport plays a crucial
role. This mechanism gives an interpretation for the recent experiment of
CuGeO_3, where the thermal conductivity depends on the crystal direction.Comment: 4 pages, 2 figure
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
Π₯ΠΠΠΠ― Π Π€Π£ΠΠΠ¦ΠΠΠΠΠΠ¬ΠΠ«Π ΠΠΠ’ΠΠ ΠΠΠΠ«. ΠΠΠ£Π§ΠΠΠ― Π¨ΠΠΠΠ ΠΠΠΠΠΠΠΠΠ Π€. Π. ΠΠ£ΠΠΠΠ¦ΠΠΠ
The paper presents a wide range of problems associated with the formation, development and practical implementation of research in materials science, carried out under direct leadership of Academician F. A. Kuznetsov by the team of researchers from the Nikolaev Institute of Inorganic Chemistry SB RAS. It shows the fruitfulness of his ideas of complex physicochemical research into each stage of the preparation of material from the precursor to the finished specific device element. Attention is drawn to his accurate prediction of the importance of selectable objects of study, his ability to correlate ongoing research with urgent global issues such as electronics, computer science, energy and photovoltaics and his skill to rally the team with a common idea and encourage active participation in the development of science both in Russia and internationally while remaining the main driving force of conducted advanced work. The paper is written in the memory of the eminent person, organizer of science, scientist and patriot whose work has always been focused on breakthrough technologies that ensure the prosperity and security of the Motherland.Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½ ΡΠΈΡΠΎΠΊΠΈΠΉ ΠΊΡΡΠ³ ΠΏΡΠΎΠ±Π»Π΅ΠΌ, ΡΠ²ΡΠ·Π°Π½Π½ΡΡ
ΡΠΎ ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΈΠ΅ΠΌ, ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ΠΌ ΠΈ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠ΅ΠΉ Π½Π°ΡΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ, Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π½ΡΡ
ΠΊΠΎΠ»Π»Π΅ΠΊΡΠΈΠ²ΠΎΠΌ ΡΠΎΡΡΡΠ΄Π½ΠΈΠΊΠΎΠ² ΠΠ½ΡΡΠΈΡΡΡΠ° Π½Π΅ΠΎΡΠ³Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ Ρ
ΠΈΠΌΠΈΠΈ ΠΈΠΌ. Π. Π. ΠΠΈΠΊΠΎΠ»Π°Π΅Π²Π° Π‘Π Π ΠΠ ΠΏΠΎΠ΄ ΡΡΠΊΠΎΠ²ΠΎΠ΄ΡΡΠ²ΠΎΠΌ Π°ΠΊΠ°Π΄Π΅ΠΌΠΈΠΊΠ° Π€. Π. ΠΡΠ·Π½Π΅ΡΠΎΠ²Π°. ΠΠΎΠΊΠ°Π·Π°Π½Π° ΠΏΠ»ΠΎΠ΄ΠΎΡΠ²ΠΎΡΠ½ΠΎΡΡΡ Π΅Π³ΠΎ ΠΈΠ΄Π΅ΠΈ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠ·ΠΈΠΊΠΎ-Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ·ΡΡΠ΅Π½ΠΈΡ ΠΊΠ°ΠΆΠ΄ΠΎΠΉ ΡΡΠ°Π΄ΠΈΠΈ ΠΏΡΠΈΠ³ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΡ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π°: ΠΎΡ ΠΏΡΠ΅Π΄ΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΈΠΊΠ° ΠΊ Π³ΠΎΡΠΎΠ²ΠΎΠΌΡ ΡΠ»Π΅ΠΌΠ΅Π½ΡΡ ΠΊΠΎΠ½ΠΊΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΡΡΡΡΠΎΠΉΡΡΠ²Π°. ΠΡΠΌΠ΅ΡΠ΅Π½ΠΎ Π΅Π³ΠΎ Π±Π΅Π·ΠΎΡΠΈΠ±ΠΎΡΠ½ΠΎΠ΅ ΠΏΡΠ΅Π΄Π²ΠΈΠ΄Π΅Π½ΠΈΠ΅ Π·Π½Π°ΡΠΈΠΌΠΎΡΡΠΈ Π²ΡΠ±ΠΈΡΠ°Π΅ΠΌΡΡ
ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠ² ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ, Π΅Π³ΠΎ ΡΠΌΠ΅Π½ΠΈΠ΅ ΡΠ²ΡΠ·ΡΠ²Π°ΡΡ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠΌΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Ρ ΡΠ°ΠΊΠΈΠΌΠΈ Π½Π°ΡΡΡΠ½ΡΠΌΠΈ ΠΈ Π³Π»ΠΎΠ±Π°Π»ΡΠ½ΡΠΌΠΈ ΠΏΡΠΎΠ±Π»Π΅ΠΌΠ°ΠΌΠΈ, ΠΊΠ°ΠΊ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΈΠΊΠ°, ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΊΠ°, ΡΠ½Π΅ΡΠ³Π΅ΡΠΈΠΊΠ°, ΡΠΎΡΠΎΠ²ΠΎΠ»ΡΡΠ°ΠΈΠΊΠ°, Π° ΡΠ°ΠΊΠΆΠ΅ Π΅Π³ΠΎ ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΡ ΡΠΏΠ»Π°ΡΠΈΠ²Π°ΡΡ ΠΊΠΎΠ»Π»Π΅ΠΊΡΠΈΠ² ΠΎΠ±ΡΠ΅ΠΉ ΠΈΠ΄Π΅Π΅ΠΉ ΠΈ Π°ΠΊΡΠΈΠ²Π½ΠΎΠ΅ ΡΡΠ°ΡΡΠΈΠ΅ Π² ΡΠ°Π·Π²ΠΈΡΠΈΠΈ ΠΊΠ°ΠΊ ΡΠΎΡΡΠΈΠΉΡΠΊΠΎΠΉ, ΡΠ°ΠΊ ΠΈ ΠΌΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠΉ Π½Π°ΡΠΊΠΈ, ΠΎΡΡΠ°Π²Π°ΡΡΡ ΠΏΡΠΈ ΡΡΠΎΠΌ Π»ΠΎΠΊΠΎΠΌΠΎΡΠΈΠ²ΠΎΠΌ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠΌΡΡ
ΠΏΠ΅ΡΠ΅Π΄ΠΎΠ²ΡΡ
ΡΠ°Π±ΠΎΡ. Π‘ΡΠ°ΡΡΡ Π½Π°ΠΏΠΈΡΠ°Π½Π° Π² ΠΏΠ°ΠΌΡΡΡ ΠΎ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ΅, ΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΎΡΠ΅ Π½Π°ΡΠΊΠΈ, ΡΡΠ΅Π½ΠΎΠΌ ΠΈ ΠΏΠ°ΡΡΠΈΠΎΡΠ΅, ΡΡΡ Π΄Π΅ΡΡΠ΅Π»ΡΠ½ΠΎΡΡΡ Π²ΡΠ΅Π³Π΄Π° Π±ΡΠ»Π° Π½Π°ΡΠ΅Π»Π΅Π½Π° Π½Π° ΠΏΡΠΎΡΡΠ²Π½ΡΠ΅ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ, ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°ΡΡΠΈΠ΅ ΠΏΡΠΎΡΠ²Π΅ΡΠ°Π½ΠΈΠ΅ ΠΈ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΡ Π ΠΎΠ΄ΠΈΠ½Ρ
Theory of Two-Dimensional Quantum Heisenberg Antiferromagnets with a Nearly Critical Ground State
We present the general theory of clean, two-dimensional, quantum Heisenberg
antiferromagnets which are close to the zero-temperature quantum transition
between ground states with and without long-range N\'{e}el order. For
N\'{e}el-ordered states, `nearly-critical' means that the ground state
spin-stiffness, , satisfies , where is the
nearest-neighbor exchange constant, while `nearly-critical' quantum-disordered
ground states have a energy-gap, , towards excitations with spin-1,
which satisfies . Under these circumstances, we show that the
wavevector/frequency-dependent uniform and staggered spin susceptibilities, and
the specific heat, are completely universal functions of just three
thermodynamic parameters. Explicit results for the universal scaling functions
are obtained by a expansion on the quantum non-linear sigma model,
and by Monte Carlo simulations. These calculations lead to a variety of
testable predictions for neutron scattering, NMR, and magnetization
measurements. Our results are in good agreement with a number of numerical
simulations and experiments on undoped and lightly-doped .Comment: 81 pages, REVTEX 3.0, smaller updated version, YCTP-xxx
- β¦