188 research outputs found

    Competition of Mesoscales and Crossover to Tricriticality in Polymer Solutions

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    We show that the approach to asymptotic fluctuation-induced critical behavior in polymer solutions is governed by a competition between a correlation length diverging at the critical point and an additional mesoscopic length-scale, the radius of gyration. Accurate light-scattering experiments on polystyrene solutions in cyclohexane with polymer molecular weights ranging from 200,000 up to 11.4 million clearly demonstrate a crossover between two universal regimes: a regime with Ising asymptotic critical behavior, where the correlation length prevails, and a regime with tricritical theta-point behavior determined by a mesoscopic polymer-chain length.Comment: 4 pages in RevTeX with 4 figure

    Universality versus nonuniversality in asymmetric fluid criticality

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    Critical phenomena in real fluids demonstrate a combination of universal features caused by the divergence of long-range fluctuations of density and nonuniversal (system-dependent) features associated with specific intermolecular interactions. Asymptotically, all fluids belong to the Ising-model class of universality. The asymptotic power laws for the thermodynamic properties are described by two independent universal critical exponents and two independent nonuniversal critical amplitudes; other critical amplitudes can be obtained by universal relations. The nonuniversal critical parameters (critical temperature, pressure, and density) can be absorbed in the property units. Nonasymptotic critical behavior of fluids can be divided in two parts, symmetric ("Ising-like") and asymmetric ("fluid-like"). The symmetric nonasymptotic behavior contains a new universal exponent (Wegner exponent) and the system-dependent crossover scale (Ginzburg number) associated with the range of intermolecular interactions, while the asymmetric features are generally described by an additional universal exponent and by three nonasymptotic amplitudes associated with mixing of the physical fields into the scaling fields.ΠšΡ€ΠΈΡ‚ΠΈΡ‡Π½i явища Π² Ρ€Π΅Π°Π»ΡŒΠ½ΠΈΡ… ΠΏΠ»ΠΈΠ½Π°Ρ… Π΄Π΅ΠΌΠΎΠ½ΡΡ‚Ρ€ΡƒΡŽΡ‚ΡŒ ΠΊΠΎΠΌΠ±iΠ½Π°Ρ†iю ΡƒΠ½iΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½ΠΈΡ… рис, спричинСних Ρ€ΠΎΠ·Π±iΠΆΠ½iΡΡ‚ΡŽ далСкосяТних Ρ„Π»ΡƒΠΊΡ‚ΡƒΠ°Ρ†iΠΉ густини, i Π½Π΅ΡƒΠ½iΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½ΠΈΡ… (систСмо Π·Π°Π»Π΅ΠΆΠ½ΠΈΡ…) рис, пов’язаних iΠ· спСцифiΡ‡Π½ΠΈΠΌΠΈ ΠΌiТмолСкулярними Π²Π·Π°Ρ”ΠΌΠΎΠ΄iями. Асимптотично всi ΠΏΠ»ΠΈΠ½ΠΈ Π½Π°Π»Π΅ΠΆΠ°Ρ‚ΡŒ Π΄ΠΎ класу ΡƒΠ½iΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½ΠΎΡΡ‚i ΠΌΠΎΠ΄Π΅Π»i IΠ·ΠΈΠ½Π³Π°. Асимптотичнi стСпСнСвi Π·Π°ΠΊΠΎΠ½ΠΈ для Ρ‚Π΅Ρ€ΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌiΡ‡Π½ΠΈΡ… властивостСй ΠΎΠΏΠΈΡΡƒΡŽΡ‚ΡŒΡΡ Π΄Π²ΠΎΠΌΠ° Π½Π΅Π·Π°Π»Π΅ΠΆΠ½ΠΈΠΌΠΈ ΡƒΠ½iΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½ΠΈΠΌΠΈ ΠΊΡ€ΠΈΡ‚ΠΈΡ‡Π½ΠΈΠΌΠΈ ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊΠ°ΠΌΠΈ i Π΄Π²ΠΎΠΌΠ° Π½Π΅Π·Π°Π»Π΅ΠΆΠ½ΠΈΠΌΠΈ Π½Π΅ΡƒΠ½iΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½ΠΈΠΌΠΈ ΠΊΡ€ΠΈΡ‚ΠΈΡ‡Π½ΠΈΠΌΠΈ Π°ΠΌΠΏΠ»iΡ‚ΡƒΠ΄Π°ΠΌΠΈ; Ρ€Π΅ΡˆΡ‚Ρƒ ΠΊΡ€ΠΈΡ‚ΠΈΡ‡Π½ΠΈΡ… Π°ΠΌΠΏΠ»iΡ‚ΡƒΠ΄ ΠΌΠΎΠΆΠ½Π° ΠΎΡ‚Ρ€ΠΈΠΌΠ°Ρ‚ΠΈ Π· ΡƒΠ½iΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½ΠΈΡ… спiΠ²Π²iдношСнь. НС-ΡƒΠ½iΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½i ΠΊΡ€ΠΈΡ‚ΠΈΡ‡Π½i ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΈ (ΠΊΡ€ΠΈΡ‚ΠΈΡ‡Π½Π° Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π°, тиск i густина) ΠΌΠΎΠΆΡƒΡ‚ΡŒ Π±ΡƒΡ‚ΠΈ Π²ΠΊΠ»ΡŽΡ‡Π΅Π½i Π² ΠΎΠ΄ΠΈΠ½ΠΈΡ†i Ρ†ΠΈΡ… властивостСй. НСасимптотичну ΠΊΡ€ΠΈΡ‚ΠΈΡ‡Π½Ρƒ ΠΏΠΎΠ²Π΅Π΄iΠ½ΠΊΡƒ ΠΏΠ»ΠΈΠ½iΠ² ΠΌΠΎΠΆΠ½Π° ΠΏΠΎΠ΄iΠ»ΠΈΡ‚ΠΈ Π½Π° Π΄Π²i частини, симСтричну (β€œiΠ·ΠΈΠ½Π³ΠΎΠΏΠΎΠ΄iбну”) i асимСтричну (β€œΠΏΠ»ΠΈΠ½ΠΎΠΏΠΎΠ΄iбну”). Π‘ΠΈΠΌΠ΅Ρ‚Ρ€ΠΈΡ‡Π½Π° нСасимптотична ΠΏΠΎΠ²Π΅Π΄iΠ½ΠΊΠ° ΠΌiΡΡ‚ΠΈΡ‚ΡŒ Π½ΠΎΠ²ΠΈΠΉ ΡƒΠ½iΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½ΠΈΠΉ ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊ (ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊ Π’Π΅Π³Π½Π΅Ρ€Π°) i систСмо Π·Π°Π»Π΅ΠΆΠ½ΠΈΠΉ ΠΌΠ°ΡΡˆΡ‚Π°Π± кросовСру (число Π“iΠ½Π·-Π±ΡƒΡ€Π³Π°), пов’язаний Π· ΠΎΠ±Π»Π°ΡΡ‚ΡŽ Π΄iΡ— ΠΌiТмолСкулярних Π²Π·Π°Ρ”ΠΌΠΎΠ΄iΠΉ, Ρ‚ΠΎΠ΄i як асимСтричнi риси Π²Π·Π°Π³Π°Π»ΡŒΠ½ΠΎΠΌΡƒ ΠΎΠΏΠΈΡΡƒΡŽΡ‚ΡŒΡΡ Π΄ΠΎΠ΄Π°Ρ‚ΠΊΠΎΠ²ΠΈΠΌ ΡƒΠ½iΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½ΠΈΠΌ ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊΠΎΠΌ i Ρ‚Ρ€ΡŒΠΎΠΌΠ° нСасимптотичними Π°ΠΌΠΏΠ»iΡ‚ΡƒΠ΄Π°ΠΌΠΈ, пов’язаними Π·i Π·ΠΌiΡˆΡƒΠ²Π°Π½Π½ΡΠΌ Ρ„iΠ·ΠΈΡ‡Π½ΠΈΡ… ΠΏΠΎΠ»iΠ² Ρƒ скСйлiΠ½Π³ΠΎΠ²ΠΈΡ… полях

    Shape of crossover between mean-field and asymptotic critical behavior in a three-dimensional Ising lattice

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    Recent numerical studies of the susceptibility of the three-dimensional Ising model with various interaction ranges have been analyzed with a crossover model based on renormalization-group matching theory. It is shown that the model yields an accurate description of the crossover function for the susceptibility.Comment: 4 pages RevTeX + 3 PostScript figures. Uses epsf.sty and rotate.sty. Final version; accepted for publication in Physics Letters

    The influence of the rare earth ions radii on the Low Spin to Intermediate Spin state transition in lanthanide cobaltite perovskites: LaCoO3 vs. HoCoO3

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    We present first principles LDA+U calculations of electronic structure and magnetic state for LaCoO3 and HoCoO3. Low Spin to Intermediate Spin state transition was found in our calculations using experimental crystallographic data for both materials with a much higher transition temperature for HoCoO3, which agrees well with the experimental estimations. Low Spin state t6e0 (non-magnetic) to Intermediate Spin state t5e1 (magnetic) transition of Co(3+) ions happens due to the competition between crystal field t_2g-e_g splitting and effective exchange interaction between 3dd spin-orbitals. We show that the difference in crystal structure parameters for HoCoO3 and LaCoO3 due to the smaller ionic radius of Ho ion comparing with La ion results in stronger crystal field splitting for HoCoO3 (0.09 eV ~ 1000 K larger than for LaCoO3) and hence tip the balance between the Low Spin and Intermediate Spin states to the non-magnetic solution in HoCoO3.Comment: 13 pages, 6 figure

    Influence of the external magnetic field on the cylindrical electron bunch injected into plasma

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    Dynamics of the initially cylindrical electron bunch injected into plasma along the external magnetic field was studied via PIC simulation. Time evolution of the spatial distributions of electric field, magnetic field and bunch electron density is analyzed. The influence of the external magnetic field on the bunch shape and wake field excitation is treated. The correlation between azimuthal magnetic field distribution and wake field shape is discussed.Π‘ ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ числСнного модСлирования ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ частиц Π² ячСйках исслСдуСтся Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ° сгустка элСктронов, ΠΈΠ·Π½Π°Ρ‡Π°Π»ΡŒΠ½ΠΎ ΠΈΠΌΠ΅ΡŽΡ‰Π΅Π³ΠΎ Ρ„ΠΎΡ€ΠΌΡƒ Ρ†ΠΈΠ»ΠΈΠ½Π΄Ρ€Π°, Π²Π»Π΅Ρ‚Π°ΡŽΡ‰Π΅Π³ΠΎ Π² ΠΏΠ»Π°Π·ΠΌΡƒ Π² присутствии ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ внСшнСго ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠ³ΠΎ поля. ΠΠ½Π°Π»ΠΈΠ·ΠΈΡ€ΡƒΡŽΡ‚ΡΡ измСнСния пространствСнных распрСдСлСний элСктричСского ΠΈ ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Π΅ΠΉ, Π° Ρ‚Π°ΠΊΠΆΠ΅ плотности элСктронов Π² сгусткС. ΠžΠ±ΡΡƒΠΆΠ΄Π°Π΅Ρ‚ΡΡ влияниС ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠ³ΠΎ поля Π½Π° Ρ„ΠΎΡ€ΠΌΡƒ сгустка ΠΈ Π²ΠΎΠ·Π±ΡƒΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΊΠΈΠ»ΡŒΠ²Π°Ρ‚Π΅Ρ€Π½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ‹. Π˜ΡΡΠ»Π΅Π΄ΡƒΠ΅Ρ‚ΡΡ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ ΠΌΠ΅ΠΆΠ΄Ρƒ Ρ„ΠΎΡ€ΠΌΠΎΠΉ сгустка, ΠΏΠΎΠ»Π΅ΠΌ ΠΊΠΈΠ»ΡŒΠ²Π°Ρ‚Π΅Ρ€Π½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ‹ ΠΈ распрСдСлСниСм Π°Π·ΠΈΠΌΡƒΡ‚Π°Π»ΡŒΠ½ΠΎΠΉ ΡΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‰Π΅ΠΉ ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠ³ΠΎ поля.Π—Π° допомогою Ρ‡ΠΈΡΠ΅Π»ΡŒΠ½ΠΎΠ³ΠΎ модСлювання ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ частинок Ρƒ ΠΊΠΎΠΌΡ–Ρ€ΠΊΠ°Ρ… Π΄ΠΎΡΠ»Ρ–Π΄ΠΆΡƒΡ”Ρ‚ΡŒΡΡ Π΄ΠΈΠ½Π°ΠΌΡ–ΠΊΠ° згустка Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π², Ρ‰ΠΎ ΠΏΠΎΡ‡Π°Ρ‚ΠΊΠΎΠ²ΠΎ ΠΌΠ°Ρ” Ρ†ΠΈΠ»Ρ–Π½Π΄Ρ€ΠΈΡ‡Π½Ρƒ Ρ„ΠΎΡ€ΠΌΡƒ, Ρ‚Π° Π²Π»Ρ–Ρ‚Π°Ρ” Π² ΠΏΠ»Π°Π·ΠΌΡƒ Ρƒ присутності Π·ΠΎΠ²Π½Ρ–ΡˆΠ½ΡŒΠΎΠ³ΠΎ поздовТнього ΠΌΠ°Π³Π½Ρ–Ρ‚Π½ΠΎΠ³ΠΎ поля. ΠΠ½Π°Π»Ρ–Π·ΡƒΡŽΡ‚ΡŒΡΡ Π·ΠΌΡ–Π½ΠΈ просторового Ρ€ΠΎΠ·ΠΏΠΎΠ΄Ρ–Π»Ρƒ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΎΠ³ΠΎ Ρ‚Π° ΠΌΠ°Π³Π½Ρ–Ρ‚Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ–Π², Π° Ρ‚Π°ΠΊΠΎΠΆ густини Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π² Ρƒ згустку. ΠžΠ±Π³ΠΎΠ²ΠΎΡ€ΡŽΡ”Ρ‚ΡŒΡΡ Π²ΠΏΠ»ΠΈΠ² Π·ΠΎΠ²Π½Ρ–ΡˆΠ½ΡŒΠΎΠ³ΠΎ ΠΌΠ°Π³Π½Ρ–Ρ‚Π½ΠΎΠ³ΠΎ поля Π½Π° Ρ„ΠΎΡ€ΠΌΡƒ згустка Ρ‚Π° Π·Π±ΡƒΠ΄ΠΆΡƒΠ²Π°Π½Ρƒ ΠΊΡ–Π»ΡŒΠ²Π°Ρ‚Π΅Ρ€Π½Ρƒ Ρ…Π²ΠΈΠ»ΡŽ. Показана Π·Π°Π»Π΅ΠΆΠ½Ρ–ΡΡ‚ΡŒ ΠΌΡ–ΠΆ Ρ„ΠΎΡ€ΠΌΠΎΡŽ згустка, ΠΏΠΎΠ»Π΅ΠΌ ΠΊΡ–Π»ΡŒΠ²Π°Ρ‚Π΅Ρ€Π½ΠΎΡ— Ρ…Π²ΠΈΠ»Ρ– Ρ‚Π° Ρ€ΠΎΠ·ΠΏΠΎΠ΄Ρ–Π»ΠΎΠΌ Π°Π·ΠΈΠΌΡƒΡ‚Π°Π»ΡŒΠ½ΠΎΡ— складової ΠΌΠ°Π³Π½Ρ–Ρ‚Π½ΠΎΠ³ΠΎ поля

    The semileptonic decays of the B_c meson

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    We study the semileptonic transitions B_c to \eta_c, J/\psi, D, D^*, B, B^*, B_s, B_s^* in the framework of a relativistic constituent quark model. We use experimental data on leptonic J/\psi decay, lattice and QCD sum rule results on leptonic B_c decay, and on radiative \eta_c transitions to adjust the quark model parameters. We compute all form factors of the above semileptonic B_c-transitions and give predictions for various semileptonic B_c decay modes including their \tau-modes when they are kinematically accessible. The implications of heavy quark symmetry for the semileptonic decays are discussed and are shown to be manifest in our explicit relativistic quark model calculation. A comparison of our results with the results of other calculations is performed.Comment: 31 pages Latex (uses epsf, revtex). Section II expanded, typos corrected. This version will appear in Phys. Rev.

    Brane World Susy Breaking from String/M Theory

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    String and M-theory realizations of brane world supersymmetry breaking scenarios are considered in which visible sector Standard Model fields are confined on a brane, with hidden sector supersymmetry breaking isolated on a distant brane. In calculable examples with an internal manifold of any volume the Kahler potential generically contains brane--brane non-derivative contact interactions coupling the visible and hidden sectors and is not of the no-scale sequestered form. This leads to non-universal scalar masses and without additional assumptions about flavor symmetries may in general induce dangerous sflavor violation even though the Standard Model and supersymmetry branes are physically separated. Deviations from the sequestered form are dictated by bulk supersymmetry and can in most cases be understood as arising from exchange of bulk supergravity fields between branes or warping of the internal geometry. Unacceptable visible sector tree-level tachyons arise in many models but may be avoided in certain classes of compactifications. Anomaly mediated and gaugino mediated contributions to scalar masses are sub-dominant except in special circumstances such as a flat or AdS pure five--dimensional bulk geometry without bulk vector multiplets.Comment: Latex, 83 pages, references adde

    Charge and Orbital Ordering and Spin State Transition Driven by Structural Distortion in YBaCo_2O_5

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    We have investigated electronic structures of antiferromagnetic YBaCo_2O_5 using the local spin-density approximation (LSDA) + U method. The charge and orbital ordered insulating ground state is correctly obtained with the strong on-site Coulomb interaction. Co^{2+} and Co^{3+} ions are found to be in the high spin (HS) and intermediate spin (IS) state, respectively. It is considered that the tetragonal to orthorhombic structural transition is responsible for the ordering phenomena and the spin states of Co ions. The large contribution of the orbital moment to the total magnetic moment indicates that the spin-orbit coupling is also important in YBaCo_2O_5.Comment: 4 pages including 4 figures, Submitted to Phys. Rev. Let

    Application of Minimal Subtraction Renormalization to Crossover Behavior near the 3^3He Liquid-Vapor Critical Point

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    Parametric expressions are used to calculate the isothermal susceptibility, specific heat, order parameter, and correlation length along the critical isochore and coexistence curve from the asymptotic region to crossover region. These expressions are based on the minimal-subtraction renormalization scheme within the Ο•4\phi^4 model. Using two adjustable parameters in these expressions, we fit the theory globally to recently obtained experimental measurements of isothermal susceptibility and specific heat along the critical isochore and coexistence curve, and early measurements of coexistence curve and light scattering intensity along the critical isochore of 3^3He near its liquid-vapor critical point. The theory provides good agreement with these experimental measurements within the reduced temperature range ∣tβˆ£β‰€2Γ—10βˆ’2|t| \le 2\times 10^{-2}

    Spin state and phase competition in TbBaCo_{2}O_{5.5} and the lanthanide series LnBaCo_{2}O_{5+\delta} (0<=\delta<=1)

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    A clear physics picture of TbBaCo2_{2}O5.5_{5.5} is revealed on the basis of density functional theory calculations. An antiferromagnetic (AFM) superexchange coupling between the almost high-spin Co3+^{3+} ions competes with a ferromagnetic (FM) interaction mediated by both p-d exchange and double exchange, being responsible for the observed AFM-FM transition. And the metal-insulator transition is accompanied by an xy/xz orbital-ordering transition. Moreover, this picture can be generalized to the whole lanthanide series, and it is predicted that a few room-temperature magnetoresistance materials could be found in LnBa1βˆ’x_{1-x}Ax_{x}Co2_{2}O5+Ξ΄_{5+\delta} (Ln=Ho,Er,Tm,Yb,Lu; A=Sr,Ca,Mg).Comment: 13 pages, 2 figures; to be published in Phys. Rev. B on 1st Sept. Title and Bylines are added to the revised versio
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