259 research outputs found

    First evidence for charge ordering in NaV2_2O5_5 from Raman spectroscopy

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    We argue on the basis of symmetry selection rules and Raman scattering spectra that NaV2_2O5_5 undergoes a charge ordering phase transition at Tc_c=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 V4.5+^{4.5+} to two different V4+^{4+} and V5+^{5+} states. In the low temperature phase the V4+^{4+} 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

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    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

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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

    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

    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

    Π₯ИМИЯ И Π€Π£ΠΠšΠ¦Π˜ΠžΠΠΠ›Π¬ΠΠ«Π• ΠœΠΠ’Π•Π Π˜ΠΠ›Π«. НАУЧНАЯ Π¨ΠšΠžΠ›Π ΠΠšΠΠ”Π•ΠœΠ˜ΠšΠ Π€. А. ΠšΠ£Π—ΠΠ•Π¦ΠžΠ’Π

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    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.РассмотрСн ΡˆΠΈΡ€ΠΎΠΊΠΈΠΉ ΠΊΡ€ΡƒΠ³ ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌ, связанных со становлСниСм, Ρ€Π°Π·Π²ΠΈΡ‚ΠΈΠ΅ΠΌ ΠΈ практичСской Ρ€Π΅Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠ΅ΠΉ Π½Π°ΡƒΡ‡Π½Ρ‹Ρ… исслСдований Π² области матСриаловСдСния, Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π½Ρ‹Ρ… ΠΊΠΎΠ»Π»Π΅ΠΊΡ‚ΠΈΠ²ΠΎΠΌ сотрудников Π˜Π½ΡΡ‚ΠΈΡ‚ΡƒΡ‚Π° нСорганичСской Ρ…ΠΈΠΌΠΈΠΈ ΠΈΠΌ. А. Π’. НиколаСва БО РАН ΠΏΠΎΠ΄ руководством Π°ΠΊΠ°Π΄Π΅ΠΌΠΈΠΊΠ° Π€. А. ΠšΡƒΠ·Π½Π΅Ρ†ΠΎΠ²Π°. Показана ΠΏΠ»ΠΎΠ΄ΠΎΡ‚Π²ΠΎΡ€Π½ΠΎΡΡ‚ΡŒ Π΅Π³ΠΎ ΠΈΠ΄Π΅ΠΈ комплСксного Ρ„ΠΈΠ·ΠΈΠΊΠΎ-химичСского изучСния ΠΊΠ°ΠΆΠ΄ΠΎΠΉ стадии приготовлСния ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π°: ΠΎΡ‚ ΠΏΡ€Π΅Π΄ΡˆΠ΅ΡΡ‚Π²Π΅Π½Π½ΠΈΠΊΠ° ΠΊ Π³ΠΎΡ‚ΠΎΠ²ΠΎΠΌΡƒ элСмСнту ΠΊΠΎΠ½ΠΊΡ€Π΅Ρ‚Π½ΠΎΠ³ΠΎ устройства. ΠžΡ‚ΠΌΠ΅Ρ‡Π΅Π½ΠΎ Π΅Π³ΠΎ Π±Π΅Π·ΠΎΡˆΠΈΠ±ΠΎΡ‡Π½ΠΎΠ΅ ΠΏΡ€Π΅Π΄Π²ΠΈΠ΄Π΅Π½ΠΈΠ΅ значимости Π²Ρ‹Π±ΠΈΡ€Π°Π΅ΠΌΡ‹Ρ… ΠΎΠ±ΡŠΠ΅ΠΊΡ‚ΠΎΠ² исслСдования, Π΅Π³ΠΎ ΡƒΠΌΠ΅Π½ΠΈΠ΅ ΡΠ²ΡΠ·Ρ‹Π²Π°Ρ‚ΡŒ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠΌΡ‹Π΅ исслСдования с Ρ‚Π°ΠΊΠΈΠΌΠΈ насущными ΠΈ Π³Π»ΠΎΠ±Π°Π»ΡŒΠ½Ρ‹ΠΌΠΈ ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΠ°ΠΌΠΈ, ΠΊΠ°ΠΊ элСктроника, ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ‚ΠΈΠΊΠ°, энСргСтика, Ρ„ΠΎΡ‚ΠΎΠ²ΠΎΠ»ΡŒΡ‚Π°ΠΈΠΊΠ°, Π° Ρ‚Π°ΠΊΠΆΠ΅ Π΅Π³ΠΎ ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡ‚ΡŒ ΡΠΏΠ»Π°Ρ‡ΠΈΠ²Π°Ρ‚ΡŒ ΠΊΠΎΠ»Π»Π΅ΠΊΡ‚ΠΈΠ² ΠΎΠ±Ρ‰Π΅ΠΉ ΠΈΠ΄Π΅Π΅ΠΉ ΠΈ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠ΅ участиС Π² Ρ€Π°Π·Π²ΠΈΡ‚ΠΈΠΈ ΠΊΠ°ΠΊ российской, Ρ‚Π°ΠΊ ΠΈ ΠΌΠ΅ΠΆΠ΄ΡƒΠ½Π°Ρ€ΠΎΠ΄Π½ΠΎΠΉ Π½Π°ΡƒΠΊΠΈ, ΠΎΡΡ‚Π°Π²Π°ΡΡΡŒ ΠΏΡ€ΠΈ этом Π»ΠΎΠΊΠΎΠΌΠΎΡ‚ΠΈΠ²ΠΎΠΌ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠΌΡ‹Ρ… ΠΏΠ΅Ρ€Π΅Π΄ΠΎΠ²Ρ‹Ρ… Ρ€Π°Π±ΠΎΡ‚. Π‘Ρ‚Π°Ρ‚ΡŒΡ написана Π² ΠΏΠ°ΠΌΡΡ‚ΡŒ ΠΎ Ρ‡Π΅Π»ΠΎΠ²Π΅ΠΊΠ΅, ΠΎΡ€Π³Π°Π½ΠΈΠ·Π°Ρ‚ΠΎΡ€Π΅ Π½Π°ΡƒΠΊΠΈ, ΡƒΡ‡Π΅Π½ΠΎΠΌ ΠΈ ΠΏΠ°Ρ‚Ρ€ΠΈΠΎΡ‚Π΅, Ρ‡ΡŒΡ Π΄Π΅ΡΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ всСгда Π±Ρ‹Π»Π° Π½Π°Ρ†Π΅Π»Π΅Π½Π° Π½Π° ΠΏΡ€ΠΎΡ€Ρ‹Π²Π½Ρ‹Π΅ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ, ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰ΠΈΠ΅ ΠΏΡ€ΠΎΡ†Π²Π΅Ρ‚Π°Π½ΠΈΠ΅ ΠΈ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡ‚ΡŒ Π ΠΎΠ΄ΠΈΠ½Ρ‹

    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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