4,514 research outputs found

    Thermal reaction of Pt film with 110 GaN epilayer

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    Backscattering spectrometry, x-ray diffractometry, and scanning electron microscopy have been used to study the reaction of a thin Pt film with an epilayer of [110] GaN on [110] sapphire upon annealing at 450, 550, 650, 750, and 800 degrees C for 30 min. A Ga concentration of 2 at. % is detected by MeV He-4(++) backscattering spectrometry in the Pt layer at 550 degrees C. By x-ray diffraction, structural changes are observed already at 450 degrees C. At 650 OC, textured Ga2Pt appears as reaction product. The surface morphology exhibits instabilities by the formation of blisters at 650 degrees C and voids at 800 degrees C

    Pion mass dependence of the Kl3K_{l3} semileptonic scalar form factor within finite volume

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    We calculate the scalar semileptonic kaon decay in finite volume at the momentum transfer tm=(mK−mπ)2t_{m} = (m_{K} - m_{\pi})^2, using chiral perturbation theory. At first we obtain the hadronic matrix element to be calculated in finite volume. We then evaluate the finite size effects for two volumes with L=1.83fmL = 1.83 fm and L=2.73fmL= 2.73 fm and find that the difference between the finite volume corrections of the two volumes are larger than the difference as quoted in \cite{Boyle2007a}. It appears then that the pion masses used for the scalar form factor in ChPT are large which result in large finite volume corrections. If appropriate values for pion mass are used, we believe that the finite size effects estimated in this paper can be useful for Lattice data to extrapolate at large lattice size.Comment: 19 pages, 5 figures, accepted for publication in EPJ

    Instability of Amorphous Ru-Si-O Thin Films under Thermal Oxidation

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    Ternary films about 200 nm thick of composition Ru20Si15O65 have been synthesized by reactive rf magnetron sputtering of a Ru1Si1 target in an argon-oxygen gas. As-deposited, the films are X-ray-amorphous. Their atomic density is 8.9 × 10^22/cm^3 (5.1 g/cm^3), and their electrical resistivity is in the range of 2 mOmega cm. After annealing in dry oxygen at 600°C for 30 min, micron-sized grains of RuO2 grow out of the film and volatile RuO4 escapes. The significance of these results is discussed

    Lattice Theories with Nonlinearly Realized Chiral Symmetry

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    We present the lattice formulation of effective Lagrangians in which chiral symmetry is realized nonlinearly on the fermion fields. In this framework both the Wilson term removing unphysical doubler fermions and the fermion mass term do not break chiral symmetry. Our lattice formulation allows us to address non-perturbative questions in effective theories of baryons interacting with pions and in models involving constitutent quarks interacting with pions and gluons. With the presented methods, a system containing a non-zero density of static baryons interacting with pions can be studied on the lattice without encountering a complex action problem. This might lead to new insights into the phase diagram of strongly interacting matter at non-zero chemical potential.Comment: 3 pages, Lattice2003(chiral

    Isospin Violation in Chiral Perturbation Theory and the Decays \eta \ra \pi \ell \nu and \tau \ra \eta \pi \nu

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    I discuss isospin breaking effects within the standard model. Chiral perturbation theory presents the appropriate theoretical framework for such an investigation in the low--energy range. Recent results on the electromagnetic contributions to the masses of the pseudoscalar mesons and the Kℓ3K_{\ell 3} amplitudes are reported. Using the one--loop formulae for the ηℓ3\eta_{\ell 3} form factors, rather precise predictions for the decay rates of η→πℓΜ\eta \rightarrow \pi \ell \nu can be obtained. Finally, I present an estimate of the \tau \ra \eta \pi \nu branching ratio derived from the dominant meson resonance contributions to this decay.Comment: 10 pages, latex, one figure available upon reques

    The Goldberger -- Treiman Relation, gAg_A and gπNNg_{\pi NN} at T≠0T\neq 0

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    The Goldberger-Treiman relation is shown to persist in the chiral limit at finite temperatures to order O(T2)O(T^2). The TT dependence of gAg_A turns out to be the same as for FπF_{\pi}, gA(T)=gA(0)(1−T2/12F2)g_{A}(T)=g_{A}(0)(1-T^2/12F^2), while gπNNg_{\pi NN} is temperature independent to this order. The baryon octet D{\cal D} and F{\cal F} couplings also behave as FπF_{\pi} if only pions are massless in the pseudoscalar meson octet.Comment: 7p, NSF-ITP-93-145, BUTP-93/27, PUTP-1433, November 199

    Baryon chiral perturbation theory with virtual photons and leptons

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    We construct the general pion-nucleon SU(2) Lagrangian including both virtual photons and leptons for relativistic baryon chiral perturbation theory up to fourth order. We include the light leptons as explicit dynamical degrees of freedom by introducing new building blocks which represent these leptons.Comment: 11 page

    Contributions of order O(mquark2){\cal O}(m_{\rm quark}^2) to Kℓ3K_{\ell 3} form factors and unitarity of the CKM matrix

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    The form factors for the Kℓ3K_{\ell 3} semileptonic decay are computed to order O(p4)O(p^4) in generalized chiral perturbation theory. The main difference with the standard O(p4)O(p^4) expressions consists in contributions quadratic in quark masses, which are described by a single divergence-free low-energy constant, A3A_3. A new simultaneous analysis is presented for the CKM matrix element VusV_{us}, the ratio FK/FπF_K/F_{\pi}, Kℓ3K_{\ell 3} decay rates and the scalar form factor slope λ0\lambda_0. This framework easily accommodates the precise value for VudV_{ud} deduced from superallowed nuclear ÎČ\beta-decays

    The Decuplet Revisited in χ\chiPT

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    The paper deals with two issues. First, we explore the quantitiative importance of higher multiplets for properties of the Δ\Delta decuplet in chiral perturbation theory. In particular, it is found that the lowest order one--loop contributions from the Roper octet to the decuplet masses and magnetic moments are substantial. The relevance of these results to the chiral expansion in general is discussed. The exact values of the magnetic moments depend upon delicate cancellations involving ill--determined coupling constants. Second, we present new relations between the magnetic moments of the Δ\Delta decuplet that are independent of all couplings. They are exact at the order of the chiral expansion used in this paper.Comment: 7 pages of double column revtex, no figure

    Chiral Corrections to Lattice Calculations of Charge Radii

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    Logarithmic divergences in pion and proton charge radii associated with chiral loops are investigated to assess systematic uncertainties in current lattice determinations of charge radii. The chiral corrections offer a possible solution to the long standing problem of why present lattice calculations yield proton and pion radii which are similar in size.Comment: PostScript file only. Ten pages. Figures included. U. of MD Preprint #92-19
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