20 research outputs found

    Cosmological Origin for Cosmic Rays Above 101910^{19} eV

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    The cosmic ray spectrum at 1019eV1020eV10^{19}{\rm eV}-10^{20}{\rm eV}, reported by the Fly's Eye and the AGASA experiments, is shown to be consistent with a cosmological distribution of sources of protons, with a power law generation spectrum dlnN/dlnE=2.3±0.5{\rm d}\ln N/{\rm d}\ln E=-2.3\pm0.5 and energy production rate of 4.5±1.5×1044erg Mpc3 yr14.5\pm1.5\times10^{44}{\rm erg}\ {\rm Mpc}^{-3}\ {\rm yr}^{-1}. The two events measured above 1020eV10^{20}{\rm eV} are not inconsistent with this model. Verifying the existence of a ``black-body cutoff'', currently observed with low significance, would require 30\sim30 observation-years with existing experiments, but only 1\sim1 year with the proposed 5000 km2\sim5000\ {\rm km}^2 detectors. For a cosmological source distribution, no anisotropy is expected in the angular distribution of events with energies up to 5×1019eV\sim5\times10^{19}{\rm eV}.Comment: uuencoded gz-compressed postscript file, including 2 figures; To appear in the October 10 (1995) issue of the Ap. J. Letter

    Failure of Mean Field Theory at Large N

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    We study strongly coupled lattice QCD with NN colors of staggered fermions in 3+1 dimensions. While mean field theory describes the low temperature behavior of this theory at large NN, it fails in the scaling region close to the finite temperature second order chiral phase transition. The universal critical region close to the phase transition belongs to the 3d XY universality class even when NN becomes large. This is in contrast to Gross-Neveu models where the critical region shrinks as NN (the number of flavors) increases and mean field theory is expected to describe the phase transition exactly in the limit of infinite NN. Our work demonstrates that close to second order phase transitions infrared fluctuations can sometimes be important even when NN is strictly infinite.Comment: 4 pages, 3 figure

    De Sitter Cosmic Strings and Supersymmetry

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    We study massive spinor fields in the geometry of a straight cosmic string in a de Sitter background. We find a hidden N=2 supersymmetry in the fermionic solutions of the equations of motion. We connect the zero mode solutions to the heat-kernel regularized Witten index of the supersymmetric algebra.Comment: Version similar to the one accepted by General Relativity and Gravitatio

    Onset of Delocalization in Quasi-1D Waveguides with Correlated Surface Disorder

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    We present first analytical results on transport properties of many-mode waveguides with rough surfaces having long-range correlations. We show that propagation of waves through such waveguides reveals a quite unexpected phenomena of a complete transparency for a subset of propagating modes. These modes do not interact with each other and effectively can be described by the theory of 1D transport with correlated disorder. We also found that with a proper choice of model parameters one can arrange a perfect transparency of waveguides inside a given window of energy of incoming waves. The results may be important in view of experimental realizations of a selective transport in application to both waveguides and electron/optic nanodevices.Comment: RevTex, 4 pages, no figures, few references are adde

    Dynamical Chiral Symmetry Breaking on a Brane in Reduced QED

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    Reduced gauge theories are theories in which while gauge fields propagate in a bulk, fermion fields are localized on a brane. We study dynamical chiral symmetry breaking on a 2-brane and a 1-brane in reduced QED_{3+1}, and on a 1-brane in reduced QED_{2+1}. Since, unlike higher dimensional gauge theories, QED_{3+1} and QED_{2+1} are well defined, their reduced versions can serve as a laboratory for studying dynamics in a higher dimensional brane world. The analysis of the Schwinger-Dyson (SD) equations in these theories reveals rich and quite nontrivial dynamics in which the conformal symmetry and its breakdown play a crucial role. Explicit solutions of the SD equations in the near-critical regime are obtained and the character of the corresponding phase transition is described.Comment: PRD versio

    d_{x^2-y^2}-Wave Pairing Fluctuations and Pseudo Spin Gap in Two-Dimensional Electron Systems

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    Pseudogap phenomena of high-T_c cuprates are examined. In terms of AFM (antiferromagnetic) and dSC (d_{x^2-y^2}-wave superconducting) auxiliary fields introduced to integrate out the fermions, the effective action for 2D electron systems with AFM and dSC fluctuations is considered. By the self-consistent renormalization (SCR), the NMR relaxation rate T_1^{-1}, the spin correlation length \xi_\sigma and the pairing correlation length \xi_d are calculated. From this calculation, a mechanism of the pseudogap formation emerges as the region of dominant d-wave short-range order (SRO) over AFM-SRO. When damping for the AFM fluctuation strongly depends on the dSC correlation length through the formation of precursor singlets around (\pi,0) and (0,\pi) points in the momentum space, the pseudogap appears in a region of the normal state characterized by decreasing 1/T_1T and increasing AFM correlation length with decrease in temperature. This reproduces a characteristic feature of the pseudogap phenomena in many underdoped cuprates. When the damping becomes insensitive to the dSC correlation length, the pseudogap region shrinks as in the overdoped cuprates.Comment: 13 pages with 5 figures, submitted to J. Phys. Soc. Jpn.; figure inclusion correcte

    Lessons from QCD2(N)QCD_2 (N\to\infty): Vacuum structure, Asymptotic Series, Instantons and all that

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    We discuss two dimensional QCD(Nc)QCD (N_c\to\infty) with fermions in the fundamental as well as adjoint representation. We find factorial growth (g2Ncπ)2k(2k)!(1)k1(2π)2k\sim (g^2N_c\pi)^{2k}\frac{(2k)!(-1)^{k-1}}{(2 \pi)^{2k}} in the coefficients of the large order perturbative expansion. We argue that this behavior is related to classical solutions of the theory, instantons, thus it has nonperturbative origin. Phenomenologically such a growth is related to highly excited states in the spectrum. We also analyze the heavy-light quark system QqˉQ\bar{q} within operator product expansion (which it turns out to be an asymptotic series). Some vacuum condensates \la\bar{q}(x_{\mu}D_{\mu})^{2n}q\ra\sim (x^2)^n\cdot n! which are responsible for this factorial growth are also discussed. We formulate some general puzzles which are not specific for 2D physics, but are inevitable features of any asymptotic expansion. We resolve these apparent puzzles within QCD2QCD_2 and we speculate that analogous puzzles might occur in real 4-dimensional QCD as well.Comment: latex, 26 pages. A final version to appear in Phys. Rev.

    Neutrinos produced by ultrahigh-energy photons at high red shift

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    Some of the proposed explanations for the origin of ultrahigh-energy cosmic rays invoke new sources of energetic photons (e.g., topological defects, relic particles, etc.). At high red shift, when the cosmic microwave background has a higher temperature but the radio background is low, the ultrahigh-energy photons can generate neutrinos through pair-production of muons and pions. Neutrinos produced at high red shift by slowly evolving sources can be detected. Rapidly evolving sources of photons can be ruled out based on the existing upper limit on the neutrino flux.Comment: 4 pages, revtex; to appear in Phys. Rev. Let
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