3,809 research outputs found

    Probability Density in the Complex Plane

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    The correspondence principle asserts that quantum mechanics resembles classical mechanics in the high-quantum-number limit. In the past few years many papers have been published on the extension of both quantum mechanics and classical mechanics into the complex domain. However, the question of whether complex quantum mechanics resembles complex classical mechanics at high energy has not yet been studied. This paper introduces the concept of a local quantum probability density ρ(z)\rho(z) in the complex plane. It is shown that there exist infinitely many complex contours CC of infinite length on which ρ(z)dz\rho(z) dz is real and positive. Furthermore, the probability integral Cρ(z)dz\int_C\rho(z) dz is finite. Demonstrating the existence of such contours is the essential element in establishing the correspondence between complex quantum and classical mechanics. The mathematics needed to analyze these contours is subtle and involves the use of asymptotics beyond all orders.Comment: 38 pages, 17figure

    On subgroups in division rings of type 22

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    Let DD be a division ring with center FF. We say that DD is a {\em division ring of type 22} if for every two elements x,yD,x, y\in D, the division subring F(x,y)F(x, y) is a finite dimensional vector space over FF. In this paper we investigate multiplicative subgroups in such a ring.Comment: 10 pages, 0 figure

    Seesaw Right Handed Neutrino as the Sterile Neutrino for LSND

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    We show that a double seesaw framework for neutrino masses with μτ\mu-\tau exchange symmetry can lead to one of the righthanded seesaw partners of the light neutrinos being massless. This can play the role of a light sterile neutrino, giving a 3+13+1 model that explains the LSND results. We get a very economical scheme, which makes it possible to predict the full 4×44\times 4 neutrino mass matrix if CP is conserved. Once CP violation is included, effect of the LSND mass range sterile neutrino is to eliminate the lower bound on neutrinoless double beta decay rate which exists for the three neutrino case with inverted mass hierarchy. The same strategy can also be used to generate a natural 3+23+2 model for LSND, which is also equally predictive for the CP conserving case in the limit of exact μτ\mu-\tau symmetry.Comment: 13 pages and one figure; model extended to 3+2 cas

    Complex Correspondence Principle

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    Quantum mechanics and classical mechanics are two very different theories, but the correspondence principle states that quantum particles behave classically in the limit of high quantum number. In recent years much research has been done on extending both quantum mechanics and classical mechanics into the complex domain. This letter shows that these complex extensions continue to exhibit a correspondence, and that this correspondence becomes more pronounced in the complex domain. The association between complex quantum mechanics and complex classical mechanics is subtle and demonstrating this relationship prequires the use of asymptotics beyond all orders.Comment: 4 pages, 6 figure

    A Comprehensive View of a Strongly Lensed Planck-Associated Submillimeter Galaxy

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    We present high-resolution maps of stars, dust, and molecular gas in a strongly lensed submillimeter galaxy (SMG) at z = 3.259. HATLAS J114637.9–001132 is selected from the Herschel-Astrophysical Terahertz Large Area Survey (H-ATLAS) as a strong lens candidate mainly based on its unusually high 500 μm flux density (~300 mJy). It is the only high-redshift Planck detection in the 130 deg^2 H-ATLAS Phase-I area. Keck Adaptive Optics images reveal a quadruply imaged galaxy in the K band while the Submillimeter Array and the Jansky Very Large Array show doubly imaged 880 μm and CO(1→0) sources, indicating differentiated distributions of the various components in the galaxy. In the source plane, the stars reside in three major kpc-scale clumps extended over ~1.6 kpc, the dust in a compact (~1 kpc) region ~3 kpc north of the stars, and the cold molecular gas in an extended (~7 kpc) disk ~5 kpc northeast of the stars. The emissions from the stars, dust, and gas are magnified by ~17, ~8, and ~7 times, respectively, by four lensing galaxies at z ~ 1. Intrinsically, the lensed galaxy is a warm (T_(dust) ~ 40-65 K), hyper-luminous (L_(IR) ~ 1.7 × 10^(13) L_☉; star formation rate (SFR) ~2000 M_☉ yr^(–1)), gas-rich (M_(gas)/M_(baryon) ~ 70%), young (M_(stellar)/SFR ~ 20 Myr), and short-lived (M_(gas)/SFR ~ 40 Myr) starburst. With physical properties similar to unlensed z > 2 SMGs, HATLAS J114637.9–001132 offers a detailed view of a typical SMG through a powerful cosmic microscope

    Charmless Three-body Decays of B Mesons

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    Charmless 3-body decays of B mesons are studied in the framework of the factorization approach. The nonresonant contributions arising from BP1P2B\to P_1P_2 transitions are evaluated using heavy meson chiral perturbation theory (HMChPT). The momentum dependence of nonresonant amplitudes is assumed to be in the exponential form e^{-\alpha_{NR}} p_B\cdot(p_i+p_j)} so that the HMChPT results are recovered in the soft meson limit pi,pj0p_i, p_j\to 0. In addition, we have identified another large source of the nonresonant signal in the matrix elements of scalar densities, e.g. , which can be constrained from the decay Bˉ0KSKSKS\bar B^0\to K_SK_SK_S or BKKSKSB^-\to K^-K_SK_S. The intermediate vector meson contributions to 3-body decays are identified through the vector current, while the scalar meson resonances are mainly associated with the scalar density. Their effects are described in terms of the Breit-Wigner formalism. Our main results are: (i) All KKK modes are dominated by the nonresonant background. The predicted branching ratios of K+KKS(L)K^+K^-K_{S(L)}, K+KKK^+K^-K^- and KKSKSK^-K_SK_S modes are consistent with the data within errors. (ii) Although the penguin-dominated B0K+KKSB^0\to K^+K^-K_{S} decay is subject to a potentially significant tree pollution, its effective sin2β\sin 2\beta is very similar to that of the KSKSKSK_SK_SK_S mode. However, direct CP asymmetry of the former, being of order -4%, is more prominent than the latter. (iii) For BKππB\to K\pi\pi decays, we found sizable nonresonant contributions in Kπ+πK^-\pi^+\pi^- and Kˉ0π+π\bar K^0\pi^+\pi^- modes, in agreement with the Belle measurements but larger than the BaBar result.Comment: 39 pages, 2 figures, version to appear in PR

    Supersymmetry Breaking by Type II Seesaw Assisted Anomaly Mediation

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    Anomaly mediated supersymmetry breaking (AMSB), when implemented in MSSM is known to suffer from the problem of negative slepton mass squared leading to breakdown of electric charge conservation. We show however that when MSSM is extended to explain small neutrino masses by including a pair of superheavy Higgs triplet superfields (the type II seesaw mechanism), the slepton masses can be deflected from the pure AMSB trajectory and become positive. In a simple model we present in this paper, the seesaw scale is about 10131014GeV10^{13}-10^{14}{\rm GeV}. Gauge coupling unification can be maintained by embedding the triplet to SU(5) {\bf 15}-multiplet. In this scenario, bino is the LSP and its mass is nearly degenerate with NLSP slepton when the triplet mass is right around the seesaw scale.Comment: 18 pages, 4 figures, added references, added footnote

    Natural Realizations of Seesaw in Mini-Warped Minimal SO(10)

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    The minimal SUSY SO(10) GUT models with {\bf 10}, {\bf 126} and {\bf 210} Higgs and only renormalizable couplings has been shown to provide a simple way to understand the neutrino mixings as well as the ratio Δm2/ΔmA2\Delta m^2_\odot/\Delta m^2_A in terms of quark mixing parameter θCabibbo\theta_{Cabibbo}, provided neutrino masses are described by type II seesaw formula. However, in this minimal picture, it is impossible to realize type II dominance with renormalizable couplings in 4-dimensions. We show that this problem can be cured by embedding this model into a warped 5-dimensional space time with warping between the Planck and the GUT scale, where both type II as well as mixed seesaw formulae can be realized in a natural manner without expanding the Higgs sector. These models also avoid the possible problem of threshold effects associated with large Higgs representations since the theory above the GUT scale is now strongly coupled.Comment: 20 pages and one figur
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