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Fluxmetric and magnetometric demagnetizing factors, NfNf and NmNm, for cylinders along the axial direction are numerically calculated as functions of material susceptibility χχ and the ratio γγ of length to diameter. The results have an accuracy better than 0.1% with respect to min(Nf,m,1-Nf,m)min(Nf,m,1-Nf,m) and are tabulated in the range of 0.01?γ?5000.01?γ?500 and -1?χ<∞-1?χ<. NmNm along the radial direction is evaluated with a lower accuracy from NmNm along the axis and tabulated in the range of 0.01?γ?10.01?γ?1 and -1?χ<∞-1?χ<. Some previous results are discussed and several applications are explained based on the new results.  相似文献   

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We study the electrical transport properties of a quantum point contact between a lead and a high Tc superconductor. For this, we use the Hamiltonian approach and non-equilibrium Green functions of the system. The electrical current and the shot noise are calculated with this formalism. We consider dx2−y2dx2y2, dxydxy, dx2−y2+isdx2y2+is and dxy+isdxy+is symmetries for the pair potential. Also we explore the s+−s+ and s++s++ symmetries describing the behavior of the ferropnictides superconductors. We found that for dxydxy symmetry there is not a zero bias conductance peak and for d+isd+is symmetries there is a displacement of the transport properties. From shot noise and current, the Fano factor is calculated and we found that it takes values of effective charge between e and 2e  , this is explained by the diffraction of quasiparticles in the contact. For the s+−s+ and s++s++ symmetries the results show that the electrical current and the shot noise depend on the mixing coefficient, furthermore, the effective electric charge can take values between 0 and 2e, in contrast with the results obtained for s wave superconductors.  相似文献   

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It is argued that the dominant contribution to the interaction of quark–gluon plasma at moderate T?TcT?Tc is given by the nonperturbative vacuum field correlators. Basing on that nonperturbative equation of state of quark–gluon plasma is computed and in the lowest approximation expressed in terms of absolute values of Polyakov lines for quarks and gluons Lfund(T),Ladj(T)=(Lfund)9/4Lfund(T),Ladj(T)=(Lfund)9/4 known from lattice and analytic calculations. Phase transition at any μ   is described as a transition due to vanishing of one of correlators, DE(x)DE(x), which implies the change of gluonic condensate ΔG2ΔG2. Resulting transition temperature Tc(μ)Tc(μ) is calculated in terms of ΔG2ΔG2 and Lfund(Tc)Lfund(Tc). The phase curve Tc(μ)Tc(μ) is in a good agreement with lattice data. In particular Tc(0)=0.27Tc(0)=0.27; 0.19; 0.17 GeV0.17 GeV for nf=0,2,3nf=0,2,3 and fixed ΔG2=0.0035 GeV4ΔG2=0.0035 GeV4.  相似文献   

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We construct a natural L2L2-metric on the perturbed Seiberg–Witten moduli spaces Mμ+Mμ+ of a compact 4-manifold MM, and we study the resulting Riemannian geometry of Mμ+Mμ+. We derive a formula which expresses the sectional curvature of Mμ+Mμ+ in terms of the Green operators of the deformation complex of the Seiberg–Witten equations. In case MM is simply connected, we construct a Riemannian metric on the Seiberg–Witten principal U(1)U(1) bundle P→Mμ+PMμ+ such that the bundle projection becomes a Riemannian submersion. On a Kähler surface MM, the L2L2-metric on Mμ+Mμ+ coincides with the natural Kähler metric on moduli spaces of vortices.  相似文献   

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The deviation δQWδQW of the weak charge from its standard model prediction due to the mixing of the W boson with the charged bilepton Y as well as of the Z   boson with the neutral ZZ and the real part of the non-Hermitian neutral bilepton X   in the economical 3–3–1 model is established. Additional contributions to the usual δQWδQW expression in the extra U(1)U(1) models and the left–right models are obtained. Our calculations are quite different from previous analyzes in this kind of the 3–3–1 models and give the limit on mass of the ZZ boson, the Z–ZZZ and W–YWY mixing angles with the more appropriate values: MZ>564 GeVMZ>564 GeV, −0.018<sinφ<00.018<sinφ<0 and |sinθ|<0.043|sinθ|<0.043.  相似文献   

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We demonstrate the emergence of non-Abelian fusion rules for excitations of a two dimensional lattice model built out of Abelian degrees of freedom. It can be considered as an extension of the usual toric code model on a two dimensional lattice augmented with matter fields. It consists of the usual C(Zp)C(Zp) gauge degrees of freedom living on the links together with matter degrees of freedom living on the vertices. The matter part is described by a nn dimensional vector space which we call HnHn. The ZpZp gauge particles act on the vertex particles and thus HnHn can be thought of as a C(Zp)C(Zp) module. An exactly solvable model is built with operators acting in this Hilbert space. The vertex excitations for this model are studied and shown to obey non-Abelian fusion rules. We will show this for specific values of nn and pp, though we believe this feature holds for all n>pn>p. We will see that non-Abelian anyons of the quantum double of C(S3)C(S3) are obtained as part of the vertex excitations of the model with n=6n=6 and p=3p=3. Ising anyons are obtained in the model with n=4n=4 and p=2p=2. The n=3n=3 and p=2p=2 case is also worked out as this is the simplest model exhibiting non-Abelian fusion rules. Another common feature shared by these models is that the ground states have a higher symmetry than ZpZp. This makes them possible candidates for realizing quantum computation.  相似文献   

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We report results from an experiment on the decay of the high-K isomers in 254No. We have been able to establish the decay from the known high-lying four-quasiparticle isomer, which we assign as a Kπ=16+Kπ=16+ state at an excitation energy of Ex=2.928(3) MeVEx=2.928(3) MeV. The decay of this state passes through a rotational band based on a previously unobserved state at Ex=2.012(2) MeVEx=2.012(2) MeV, which we suggest is based on a two-quasineutron configuration with Kπ=10+Kπ=10+. This state in turn decays to a rotational band based on the known Kπ=8Kπ=8 isomer, which we infer must also have a two quasineutron configuration. We are able to assign many new gamma-rays associated with the decay of the Kπ=8Kπ=8 isomer, including the identification of a highly K-forbidden ΔK=8ΔK=8 E1 transition to the ground-state band. These results provide valuable new information on the orbitals close to the Fermi surface, pairing correlations, deformation and rotational response, and K-conservation in nuclei of the deformed trans-fermium region.  相似文献   

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Considering gravitino dark matter scenarios with a long-lived charged slepton, we show that collider measurements of the slepton mass and its lifetime can probe not only the gravitino mass but also the post-inflationary reheating temperature TRTR. In a model independent way, we derive upper limits on TRTR and discuss them in light of the constraints from the primordial catalysis of 6Li through bound-state effects. In the collider-friendly region of slepton masses below 1 TeV, the obtained conservative estimate of the maximum reheating temperature is about TR=3×109 GeVTR=3×109 GeV for the limiting case of a small gluino–slepton mass splitting and about TR=108 GeVTR=108 GeV for the case that is typical for universal soft supersymmetry breaking parameters at the scale of grand unification. We find that a determination of the gluino–slepton mass ratio at the Large Hadron Collider will test the possibility of TR>109 GeVTR>109 GeV and thereby the viability of thermal leptogenesis with hierarchical heavy right-handed Majorana neutrinos.  相似文献   

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