244 research outputs found

    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

    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

    Ultrafast nonlocal control of spontaneous emission

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    Solid-state cavity quantum electrodynamics systems will form scalable nodes of future quantum networks, allowing the storage, processing and retrieval of quantum bits, where a real-time control of the radiative interaction in the cavity is required to achieve high efficiency. We demonstrate here the dynamic molding of the vacuum field in a coupled-cavity system to achieve the ultrafast nonlocal modulation of spontaneous emission of quantum dots in photonic crystal cavities, on a timescale of ~200 ps, much faster than their natural radiative lifetimes. This opens the way to the ultrafast control of semiconductor-based cavity quantum electrodynamics systems for application in quantum interfaces and to a new class of ultrafast lasers based on nano-photonic cavities.Comment: 15 pages, 4 figure

    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

    Enhancement of the Thermal Conductivity in gapped Quantum Spin Chains

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    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

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    Measurements of the thermal conductivity as a function of temperature and magnetic field in the 2D dimer spin system SrCu2_2(BO3_3)2_2 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

    Heavy-Mass Behavior of Ordered Perovskites ACu3Ru4O12 (A = Na, Ca, La)

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    We synthesized ACu3Ru4O12 (A = Na, Na0.5Ca0.5, Ca, Ca0.5La0.5, La) and measured their DC magnetization, AC susceptibility, specific heat, and resistivity, in order to investigate the effects of the hetero-valent substitution. A broad peak in the DC magnetization around 200 K was observed only in CaCu3Ru4O12, suggesting the Kondo effect due to localized Cu2+ ions. However, the electronic specific heat coefficients exhibit large values not only for CaCu3Ru4O12 but also for all the other samples. Moreover, the Wilson ratio and the Kadowaki-Woods ratio of our samples are all similar to the values of other heavy-fermion compounds. These results question the Kondo effect as the dominant origin of the mass enhancement, and rather indicate the importance of correlations among itinerant Ru electrons.Comment: 6 pages, 6 figures, to be published in J. Phys. Soc. Jp

    Theory of Two-Dimensional Quantum Heisenberg Antiferromagnets with a Nearly Critical Ground State

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    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, ρs\rho_s, satisfies ρsβ‰ͺJ\rho_s \ll J, where JJ is the nearest-neighbor exchange constant, while `nearly-critical' quantum-disordered ground states have a energy-gap, Ξ”\Delta, towards excitations with spin-1, which satisfies Ξ”β‰ͺJ\Delta \ll J. 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 1/N1/N expansion on the O(N)O(N) 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 La2βˆ’Ξ΄SrΞ΄CuO4La_{2-\delta} Sr_{\delta}Cu O_4.Comment: 81 pages, REVTEX 3.0, smaller updated version, YCTP-xxx
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