19,406 research outputs found

    Faddeev fixed-center approximation to the NKˉKN\bar{K}K system and the signature of a N(1920)(1/2+)N^*(1920)(1/2^+) state

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    We perform a calculation for the three body NKˉKN \bar{K} K scattering amplitude by using the fixed center approximation to the Faddeev equations, taking the interaction between NN and Kˉ\bar{K}, NN and KK, and Kˉ\bar{K} and KK from the chiral unitary approach. The resonant structures show up in the modulus squared of the three body scattering amplitude and suggest that a NKˉKN\bar{K}K hadron state can be formed. Our results are in agreement with others obtained in previous theoretical works, which claim a new NN^* resonance around 1920 MeV with spin-parity JP=1/2+J^P=1/2^+. The existence of these previous works allows us to test the accuracy of the fixed center approximation in the present problem and sets the grounds for possible application in similar problems, as an explorative tool to determine bound or quasibound three hadron systems.Comment: Published versio

    Plausible explanation of the Δ5/2+(2000)\Delta_{5/2^{+}}(2000) puzzle

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    From a Faddeev calculation for the π(Δρ)N5/2(1675)\pi-(\Delta\rho)_{N_{5/2^{-}}(1675)} system we show the plausible existence of three dynamically generated I(JP)=3/2(5/2+)I(J^{P})=3/2 (5/2^{+}) baryon states below 2.3 GeV whereas only two resonances, Δ5/2+(1905)()\Delta_{5/2^{+}}(1905)(\ast\ast\ast\ast) and Δ5/2+(2000)(),\Delta_{5/2^{+}}(2000)(\ast\ast), are cataloged in the Particle Data Book Review. Our results give theoretical support to data analyses extracting two distinctive resonances, Δ5/2+(1740)\Delta_{5/2^{+}}(\sim1740) and Δ5/2+(2200),\Delta_{5/2^{+}}(\sim2200), from which the mass of Δ5/2+(2000)()\Delta_{5/2^{+}}(2000)(\ast\ast) is estimated. We propose that these two resonances should be cataloged instead of Δ5/2+(2000).\Delta_{5/2^{+}}(2000). This proposal gets further support from the possible assignment of the other baryon states found in the approach in the I=1/2,3/2I=1/2,3/2 with JP=1/2+,3/2+,5/2+J^{P}=1/2^{+},3/2^{+},5/2^+ sectors to known baryonic resonances. In particular, Δ1/2+(1750)()\Delta_{1/2^{+}}(1750)(\ast) is naturally interpreted as a πN1/2(1650)\pi N_{1/2^{-}}(1650) bound state.Comment: 13 pages, 7 figure

    Theory of magnetoelastic resonance in a mono-axial chiral helimagnet

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    We study magnetoelastic resonance phenomena in a mono-axial chiral helimagnet belonging to hexagonal crystal class. By computing the spectrum of coupled elastic wave and spin wave, it is demonstrated how hybridization occurs depending on their chirality. Specific features of the magnetoelastic resonance are discussed for the conical phase and the soliton lattice phase stabilized in the mono-axial chiral helimagnet. The former phase exhibits appreciable non-reciprocity of the spectrum, the latter is characterized by a multi-resonance behavior. We propose that the non-reciprocal spin wave around the forced-ferromagnetic state has potential capability to convert the linearly polarized elastic wave to circularly polarized one with the chirality opposite to the spin wave chirality.Comment: 12 pages, 5 figures, Accepted in Phys. Rev.

    The Market Price of Credit Risk: An Empirical Analysis of Interest Rate Swap Spreads

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    This paper studies the market price of credit risk incorporated into one of the most important credit spreads in the financial markets: interest rate swap spreads. Our approach consists of jointly modeling the swap and Treasury term structures using a general five-factor affine credit framework and estimating the parameters by maximum likelihood. We solve for the implied special financing rate for Treasury bonds and find that the liquidity component of on-the-run bond prices can be significant. We also find that credit premia in swap spreads are positive on average. These premia, however, vary significantly over time and were actually negative for much of the 1990s.

    Retardation Terms in The One-Gluon Exchange Potential

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    It is pointed out that the retardation terms given in the original Fermi-Breit potential vanish in the center of mass frame. The retarded one-gluon exchange potential is rederived in this paper from the three-dimensional one-gluon exchange kernel which appears in the exact three-dimensional relativistic equation for quark-antiquark bound states. The retardation part of the potential given in the approximation of order p2/m2p^2/m^2 is shown to be different from those derived in the previous literature. This part is off-shell and does no longer vanish in the center of mass frame
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