4,408 research outputs found

    Critical point of Nf=3N_f = 3 QCD from lattice simulations in the canonical ensemble

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    A canonical ensemble algorithm is employed to study the phase diagram of Nf=3N_f = 3 QCD using lattice simulations. We lock in the desired quark number sector using an exact Fourier transform of the fermion determinant. We scan the phase space below TcT_c and look for an S-shape structure in the chemical potential, which signals the coexistence phase of a first order phase transition in finite volume. Applying Maxwell construction, we determine the boundaries of the coexistence phase at three temperatures and extrapolate them to locate the critical point. Using an improved gauge action and improved Wilson fermions on lattices with a spatial extent of 1.8 \fm and quark masses close to that of the strange, we find the critical point at TE=0.925(5)TcT_E = 0.925(5) T_c and baryon chemical potential μBE=2.60(8)Tc\mu_B^E = 2.60(8) T_c.Comment: 5 pages, 7 figures, references added, published versio

    Finite density phase transition of QCD with Nf=4N_f=4 and Nf=2N_f=2 using canonical ensemble method

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    In a progress toward searching for the QCD critical point, we study the finite density phase transition of Nf=4N_f = 4 and 2 lattice QCD at finite temperature with the canonical ensemble approach. We develop a winding number expansion method to accurately project out the particle number from the fermion determinant which greatly extends the applicable range of baryon number sectors to make the study feasible. Our lattice simulation was carried out with the clover fermions and improved gauge action. For a given temperature, we calculate the baryon chemical potential from the canonical approach to look for the mixed phase as a signal for the first order phase transition. In the case of Nf=4N_f=4, we observe an "S-shape" structure in the chemical potential-density plane due to the surface tension of the mixed phase in a finite volume which is a signal for the first order phase transition. We use the Maxwell construction to determine the phase boundaries for three temperatures below TcT_c. The intersecting point of the two extrapolated boundaries turns out to be at the expected first order transition point at TcT_c with μ=0\mu = 0. This serves as a check for our method of identifying the critical point. We also studied the Nf=2N_f =2 case, but do not see a signal of the mixed phase for temperature as low as 0.83 TcT_c.Comment: 28 pages, 11 figures,references added, final versio

    Stability of Strutinsky Shell Correction Energy in Relativistic Mean Field Theory

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    The single-particle spectrum obtained from the relativistic mean field (RMF) theory is used to extract the shell correction energy with the Strutinsky method. Considering the delicate balance between the plateau condition in the Strutinsky smoothing procedure and the convergence for the total binding energy, the proper space sizes used in solving the RMF equations are investigated in detail by taking 208Pb as an example. With the proper space sizes, almost the same shell correction energies are obtained by solving the RMF equations either on basis space or in coordinate space.Comment: 9 pages, 4 figure

    Involving Low-Pressure Plasma for Surface Pre-Treatment and Post Print Sintering of Silver Tracks on Polymer Substrates

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    A method of production conductive silver tracks on thermally sensitive polymer (BOPP) was offered, involving plasma for preprint polymer surface activation to enable better adhesion properties and postprint selective etching to reduce amounts of polymer and raise electroconductivity. Inkjet, spin coating, and roll-blade coating were the methods of application of silver nanoparticle inks. We report to achieve two magnitudes lower sheet resistance of silver thin film with no effect on polymer substrate. This method with little modification could be adopted for production of flexible electronics on highly thermally sensitive polymers. When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/3539

    Non-Abelian Medium Effects in Quark-Gluon Plasma

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    Based on the kinetic theory, the non-Abelian medium property of hot Quark-Gluon Plasma is investigated. The nonlinearity of the plasma comes from two aspects: The nonlinear wave-wave interaction and self-interaction of color field. The non-Abelian color permittivity is obtained by expanding the kinetic equations to third order. As an application, the nonlinear Landau damping rate and the nonlinear eigenfrequency shift are calculated in the longwave length limit.Comment: 12 pages(Revtex), no figure

    Symmetry breaking and manipulation of nonlinear optical modes in an asymmetric double-channel waveguide

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    We study light-beam propagation in a nonlinear coupler with an asymmetric double-channel waveguide and derive various analytical forms of optical modes. The results show that the symmetry-preserving modes in a symmetric double-channel waveguide are deformed due to the asymmetry of the two-channel waveguide, yet such a coupler supports the symmetry-breaking modes. The dispersion relations reveal that the system with self-focusing nonlinear response supports the degenerate modes, while for self-defocusingmedium the degenerate modes do not exist. Furthermore, nonlinear manipulation is investigated by launching optical modes supported in double-channel waveguide into a nonlinear uniform medium.Comment: 10 page

    A Note on Normal Forms of Quantum States and Separability

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    We study the normal form of multipartite density matrices. It is shown that the correlation matrix (CM) separability criterion can be improved from the normal form we obtained under filtering transformations. Based on CM criterion the entanglement witness is further constructed in terms of local orthogonal observables for both bipartite and multipartite systems.Comment: 8 page

    On Estimation of Fully Entangled Fraction

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    We study the fully entangled fraction (FEF) of arbitrary mixed states. New upper bounds of FEF are derived. These upper bounds make complements on the estimation of the value of FEF. For weakly mixed quantum states, an upper bound is shown to be very tight to the exact value of FEF.Comment: 8 pages, 2 figure
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