542 research outputs found

    Renormalization-group approach to the stochastic Navier--Stokes equation: Two-loop approximation

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    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 Ξ²\beta 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 dd-dimensional case is briefly discussed.Comment: 20 pages, 3 figure

    On the stability problem in the O(N) nonlinear sigma model

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    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

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    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

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    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

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    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

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    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

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    Π—Π›ΠžΠšΠΠ§Π•Π‘Π’Π’Π•ΠΠΠ«Π• ΠΠžΠ’ΠžΠžΠ‘Π ΠΠ—ΠžΠ’ΠΠΠ˜Π―ΠΠžΠ—ΠžΠ›ΠžΠ“Π˜Π§Π•Π‘ΠšΠ˜Π• ЀОРМЫ Π ΠΠšΠΠ—ΠΠ‘ΠžΠ›Π•Π’ΠΠ•ΠœΠžΠ‘Π’Π¬, ЧАБВОВА Π‘Π›Π£Π§ΠΠ•Π’Π£ΠšΠ ΠΠ˜ΠΠΠ¦Π΅Π»ΡŒ. ИсслСдованиС зависимости ΠΌΠ΅ΠΆΠ΄Ρƒ нозологичСскими Ρ„ΠΎΡ€ΠΌΠ°ΠΌΠΈ ΠΏΠ΅Ρ€Π²Ρ‹Ρ… ΠΈ Π²Ρ‚ΠΎΡ€Ρ‹Ρ… Ρ€Π°ΠΊΠΎΠ² Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ², ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΏΡ€ΠΎΡ…ΠΎΠ΄ΠΈΠ»ΠΈ ΡΠΏΠ΅Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎΠ΅ Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρƒ онкологичСского заболСвания ΠΈ Ρƒ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π²ΠΎΠ·Π½ΠΈΠΊΠ»ΠΈ Π²Ρ‚ΠΎΡ€Ρ‹Π΅ Ρ€Π°ΠΊΠΈ Ρ‡Π΅Ρ€Π΅Π· 3 Π³ΠΎΠ΄Π° ΠΈ Π±ΠΎΠ»Π΅Π΅ послС окончания лСчСния. ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π» ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. Π’ исслСдовании ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΎΡΡŒ сравнСниС ΠΌΠ΅ΠΆΠ΄Ρƒ нозологичСской структурой Π²Ρ‚ΠΎΡ€Ρ‹Ρ… Ρ€Π°ΠΊΠΎΠ², ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ Π²ΠΎΠ·Π½ΠΈΠΊΠ»ΠΈ Ρƒ 203 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ², ΠΏΡ€ΠΎΡ…ΠΎΠ΄ΠΈΠ²ΡˆΠΈΡ… Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρƒ онкологичСской ΠΏΠ°Ρ‚ΠΎΠ»ΠΎΠ³ΠΈΠΈ, ΠΈ ΠΎΡ„ΠΈΡ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ Π΄Π°Π½Π½Ρ‹ΠΌΠΈ ΠΎΠ± ΡƒΠ΄Π΅Π»ΡŒΠ½ΠΎΠΌ вСсС 10 основных нозологичСских Ρ„ΠΎΡ€ΠΌ злокачСствСнных Π½ΠΎΠ²ΠΎΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠΉ насСлСния Π£ΠΊΡ€Π°ΠΈΠ½Ρ‹. БтатистичСская Π·Π½Π°Ρ‡ΠΈΠΌΠΎΡΡ‚ΡŒ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² ΠΎΡ†Π΅Π½ΠΈΠ²Π°Π»Π°ΡΡŒ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ Π΄ΠΎΠ²Π΅Ρ€ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»ΠΎΠ², Π½ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ спСцифики ΠΊΠΎΠ½Ρ‚ΠΈΠ½Π³Π΅Π½Ρ‚Π° ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² ΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ, Π³Π΄Π΅ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΎΡΡŒ исслСдованиС. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. Π’ соотвСтствии с ΡƒΠ΄Π΅Π»ΡŒΠ½Ρ‹ΠΌ вСсом нозологичСских Ρ„ΠΎΡ€ΠΌ ΠΏΠ΅Ρ€Π²Ρ‹Ρ… Ρ€Π°ΠΊΠΎΠ², обусловлСнных, Π² ΠΏΠ΅Ρ€Π²ΡƒΡŽ ΠΎΡ‡Π΅Ρ€Π΅Π΄ΡŒ, спСциализациСй ΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ, обслСдуСмыС Π³Ρ€ΡƒΠΏΠΏΡ‹ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² Π±Ρ‹Π»ΠΈ Ρ€Π°Π·Π΄Π΅Π»Π΅Π½Ρ‹ Π½Π° 5 нозологичСских ΠΏΠΎΠ΄Π³Ρ€ΡƒΠΏΠΏ: ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ с Ρ€Π°ΠΊΠΎΠΌ ΠΌΠΎΠ»ΠΎΡ‡Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ‹, Ρ‰ΠΈΡ‚ΠΎΠ²ΠΈΠ΄Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ‹, Ρ‚Π΅Π»Π° ΠΌΠ°Ρ‚ΠΊΠΈ, шСйки ΠΌΠ°Ρ‚ΠΊΠΈ, Ρ€Π°ΠΊ яичников ΠΈ с ΠΈΠ½Ρ‹ΠΌΠΈ Ρ„ΠΎΡ€ΠΌΠ°ΠΌΠΈ Ρ€Π°ΠΊΠ°. Для ΠΊΠ°ΠΆΠ΄ΠΎΠΉ ΠΈΠ· ΠΏΠΎΠ΄Π³Ρ€ΡƒΠΏΠΏ Π±Ρ‹Π»Π° исслСдована нозологичСская структура Π²Ρ‚ΠΎΡ€Ρ‹Ρ… Ρ€Π°ΠΊΠΎΠ² ΠΈ сопоставлСна с ΠΎΠ±Ρ‰Π΅ΠΉ структурой злокачСствСнных Π½ΠΎΠ²ΠΎΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΠΎ Π΄Π°Π½Π½Ρ‹ΠΌ ΠΎΡ„ΠΈΡ†ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ статистики. Показано, Ρ‡Ρ‚ΠΎ частота пяти Π²Ρ‹Π΄Π΅Π»Π΅Π½Π½Ρ‹Ρ… нозологичСских Ρ„ΠΎΡ€ΠΌ, рассчитанных для ΠΊΠ»ΠΈΠ½ΠΈΠΊΠΈ, достаточно Ρ…ΠΎΡ€ΠΎΡˆΠΎ соотвСтствуСт популяционному срСднСму, ΠΏΡ€ΠΈ этом для Π΄Π²ΡƒΡ… Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… нозологичСских Ρ„ΠΎΡ€ΠΌ соотвСтствиС находится Π² ΠΏΡ€Π΅Π΄Π΅Π»Π°Ρ… ΠΎΠΆΠΈΠ΄Π°Π΅ΠΌΠΎΠΉ стохастичСской измСнчивости. Π’Π°ΠΊΠΈΠΌ ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ, ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ Π½Π΅ сущСствуСт статистичСски Π·Π½Π°Ρ‡ΠΈΠΌΡ‹Ρ… Ρ€Π°Π·Π»ΠΈΡ‡ΠΈΠΉ ΠΌΠ΅ΠΆΠ΄Ρƒ ΠΏΡ€ΠΎΡ†Π΅Π½Ρ‚Π½Ρ‹ΠΌ составом 10 основных нозологичСских Ρ„ΠΎΡ€ΠΌ Ρ€Π°ΠΊΠ° насСлСния Π£ΠΊΡ€Π°ΠΈΠ½Ρ‹ ΠΈ структурой нозологичСских Ρ„ΠΎΡ€ΠΌ Π²Ρ‚ΠΎΡ€Ρ‹Ρ… Ρ€Π°ΠΊΠΎΠ² Ρƒ исслСдуСмой Π³Ρ€ΡƒΠΏΠΏΡ‹ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ². Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅. НозологичСская Ρ„ΠΎΡ€ΠΌΠ° Π²Ρ‚ΠΎΡ€Ρ‹Ρ… Ρ€Π°ΠΊΠΎΠ² Π½Π΅ являСтся слСдствиСм ΠΏΠ΅Ρ€Π²ΠΎΠ³ΠΎ Ρ€Π°ΠΊΠ°, Π° воспроизводит ΠΎΠ±Ρ‰ΡƒΡŽ Π½ΠΎΠ·ΠΎΠ»ΠΎΠ³ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ структуру заболСваСмости злокачСствСнными новообразованиями.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

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    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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