542 research outputs found
Renormalization-group approach to the stochastic Navier--Stokes equation: Two-loop approximation
The field theoretic renormalization group is applied to the stochastic
Navier--Stokes equation that describes fully developed fluid turbulence. The
complete two-loop calculation of the renormalization constant, the
function, the fixed point and the ultraviolet correction exponent is performed.
The Kolmogorov constant and the inertial-range skewness factor, derived to
second order of the \eps expansion, are in a good agreement with the
experiment. The possibility of the extrapolation of the \eps expansion beyond
the threshold where the sweeping effects become important is demonstrated on
the example of a Galilean-invariant quantity, the equal-time pair correlation
function of the velocity field. The extension to the -dimensional case is
briefly discussed.Comment: 20 pages, 3 figure
On the stability problem in the O(N) nonlinear sigma model
The stability problem for the O(N) nonlinear sigma model in the 2+\epsilon
dimensions is considered. We present the results of the 1/N^{2} order
calculations of the critical exponents (in the 2<d<4 dimensions) of the
composite operators relevant for this problem. The arguments in the favor of
the scenario with the conventional fixed point are given.Comment: 9 pages, revtex, 1 Postscript figur
Premartensitic Transition in Ni2+xMn1-xGa Heusler Alloys
The temperature dependencies of the resistivity and magnetization of a series
of Ni2+XMn1-XGa (X = 0 - 0.09) alloys were investigated. Along with the
anomalies associated with ferromagnetic and martensitic transitions,
well-defined anomalies were observed at the temperature of premartensitic
transformation. The premartensitic phase existing in a temperature range 200 -
260 K in the stoichiometric Ni2MnGa is suppressed by the martensitic phase with
increasing Ni content and vanishes in Ni2.09Mn0.91Ga composition
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
O(1/N_f) Corrections to the Thirring Model in 2<d<4
The Thirring model, that is, a relativistic field theory of fermions with a
contact interaction between vector currents, is studied for dimensionalities
2<d<4 using the 1/N_f expansion, where N_f is the number of fermion species.
The model is found to have no ultraviolet divergences at leading order provided
a regularization respecting current conservation is used. Explicit O(1/N_f)
corrections are computed, and the model shown to be renormalizable at this
order in the massless limit; renormalizability appears to hold to all orders
due to a special case of Weinberg's theorem. This implies there is a universal
amplitude for four particle scattering in the asymptotic regime. Comparisons
are made with both the Gross-Neveu model and QED.Comment: 22 pages in plain TeX, with 7 figs included using psfig.tex (Minor
conceptual changes - algebra unaffected
Integral Transforms for Conformal Field Theories with a Boundary
A new method is developed for solving the conformally invariant integrals
that arise in conformal field theories with a boundary. The presence of a
boundary makes previous techniques for theories without a boundary less
suitable. The method makes essential use of an invertible integral transform,
related to the radon transform, involving integration over planes parallel to
the boundary. For successful application of this method several nontrivial
hypergeometric function relations are also derived.Comment: 20 pagess, LateX fil
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
High frequency ESR investigation on dynamical charge disproportionation and spin gap excitation in NaV_2O_5
A significant frequency dependence of the ESR line width is found in NaV_2O_5
between 34-100 K and the line width increases as the resonance frequency is
increased from 95 GHz to 760 GHz. The observed frequency dependence is
qualitatively explained in terms of the dynamical charge disproportionation.
The present results show the essential role of the internal charge degree of
freedom in a V-O-V bond. We have also proposed the existence of the
Dzyaloshinsky-Moriya interaction in the low temperature charge ordered phase
considering the breaking of the selection rule of ESR realized as the direct
observation of the spin gap excitation.Comment: 9 figures submitted to J. Phys.Soc. Jp
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