101,274 research outputs found

    Finding Exponential Product Formulas of Higher Orders

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    In the present article, we review a continual effort on generalization of the Trotter formula to higher-order exponential product formulas. The exponential product formula is a good and useful approximant, particularly because it conserves important symmetries of the system dynamics. We focuse on two algorithms of constructing higher-order exponential product formulas. The first is the fractal decomposition, where we construct higher-order formulas recursively. The second is to make use of the quantum analysis, where we compute higher-order correction terms directly. As interludes, we also have described the decomposition of symplectic integrators, the approximation of time-ordered exponentials, and the perturbational composition.Comment: 22 pages, 9 figures. To be published in the conference proceedings ''Quantum Annealing and Other Optimization Methods," eds. B.K.Chakrabarti and A.Das (Springer, Heidelberg

    Aging dynamics of ferromagnetic and reentrant spin glass phases in stage-2 Cu0.80_{0.80}C0.20_{0.20}Cl2_{2} graphite intercalation compound

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    Aging dynamics of a reentrant ferromagnet stage-2 Cu0.8_{0.8}Co0.2_{0.2}Cl2_{2} graphite intercalation compound has been studied using DC magnetic susceptibility. This compound undergoes successive transitions at the transition temperatures TcT_{c} (8.7\approx 8.7 K) and TRSGT_{RSG} (3.3\approx 3.3 K). The relaxation rate SZFC(t)S_{ZFC}(t) exhibits a characteristic peak at tcrt_{cr} below TcT_{c}. The peak time tcrt_{cr} as a function of temperature TT shows a local maximum around 5.5 K, reflecting a frustrated nature of the ferromagnetic phase. It drastically increases with decreasing temperature below TRSGT_{RSG}. The spin configuration imprinted at the stop and wait process at a stop temperature TsT_{s} (<Tc<T_{c}) during the field-cooled aging protocol, becomes frozen on further cooling. On reheating, the memory of the aging at TsT_{s} is retrieved as an anomaly of the thermoremnant magnetization at TsT_{s}. These results indicate the occurrence of the aging phenomena in the ferromagnetic phase (TRSG<T<TcT_{RSG}<T<T_{c}) as well as in the reentrant spin glass phase (T<TRSGT<T_{RSG}).Comment: 9 pages, 9 figures; submitted to Physical Review

    The Free Energy and the Scaling Function of the Ferromagnetic Heisenberg Chain in a Magnetic Field

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    A nonlinear susceptibilities (the third derivative of a magnetization mSm_S by a magnetic field hh ) of the SS=1/2 ferromagnetic Heisenberg chain and the classical Heisenberg chain are calculated at low temperatures T.T. In both chains the nonlinear susceptibilities diverge as T6T^{-6} and a linear susceptibilities diverge as T2.T^{-2}. The arbitrary spin SS Heisenberg ferromagnet [[ H=i=1N{JSiSi+1(h/S)Siz}{\cal H} = \sum_{i=1}^{N} \{ - J{\bf S}_{i} {\bf S}_{i+1} - (h/S) S_{i}^{z} \} (J>0),(J>0), ]] has a scaling relation between mS,m_S, hh and T:T: mS(T,h)=F(S2Jh/T2).m_S(T,h) = F( S^2 Jh/T^2). The scaling function F(x)F(x)=(2xx/3)-(44x3x^{3}/135) + O(x5x^{5}) is common to all values of spin S.S.Comment: 16 pages (revtex 2.0) + 6 PS figures upon reques

    Structure of the breakpoint region in CVC of the intrinsic Josephson junctions

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    A fine structure of the breakpoint region in the current-voltage characteristics of the coupled intrinsic Josephson junctions in the layered superconductors is found. We establish a correspondence between the features in the current-voltage characteristics and the character of the charge oscillations in superconducting layers in the stack and explain the origin of the breakpoint region structure.Comment: 5 pages, 5 figures. Accepted for Phys.Rev.

    Long-distance final-state interactions and J/psi decay

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    To understand the short-distance vs long-distance final-state interactions, we have performed a detailed amplitude analysis for the two-body decay, J/psi into vector and pseudoscalar mesons. The current data favor a large relative phase nearly 90 degrees between the three-gluon and one-photon decay amplitudes. The source of this phase is apparently in the long-distance final-state interaction. Nothing anomalous is found in the magnitudes of the three-gluon and one-photon amplitudes. We discuss implications of this large relative phase in the weak decay of heavy particles.Comment: 11 pages, RevTe

    A Consistent model of Electroweak data including ZbbZ\to b\overline{b} and ZccZ\to c \overline{c}

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    We have performed an overall fit to the electroweak data with the generation blind U(1)U(1) extension of the Standard Model. As input data for fitting we have included the asymmetry parameters, the particle decay widths of ZZ, neutrino scattering, and atomic parity violation. The QCD coupling αs\alpha_s has been constrained to the world average obtained from all data except the ZZ width. On the basis of our fit we have constructed a viable gauge model that not only explains RbR_b and RcR_c but also provides a much better overall fit to the data than the Standard Model. Despite its phenomenological viability, our model is unfortunately not simple from the theoretical viewpoint. Atomic parity violation experiments strongly disfavor more aesthetically appealing alternatives that can be grand unified.Comment: LaTexx, 14 page
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