2,397 research outputs found

    An upper limit on CP violation in the Bs0−Bˉs0B^0_s-\bar{B}^0_s system

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    In a previous publication we noted that the time dependence of an incoherent B0−Bˉ0B^0-\bar{B}^0 mixture undergoes a qualitative change when the magnitude of CP violation δ\delta exceeds a critical value. Requiring, on physical grounds, that the system evolve from an initial incoherent state to a final pure state in a monotonic way, yields a new upper limit for δ\delta. The recent measurement of the wrong charge semileptonic asymmetry of Bs0B_s^0 mesons presented by the D0 collaboration is outside this bound by one standard deviation. If this result is confirmed it implies the existence of a new quantum mechanical oscillation phenomenon.Comment: 7 pages, 2 figures, version submitted for publication (Physical Review

    Baryon Magnetic Moments and Proton Spin: A Model with Collective Quark Rotation

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    We analyse the baryon magnetic moments in a model that relates them to the parton spins Δu\Delta u, Δd\Delta d, Δs\Delta s, and includes a contribution from orbital angular momentum. The specific assumption is the existence of a 3-quark correlation (such as a flux string) that rotates with angular momentum ⟨Lz⟩\langle L_z \rangle around the proton spin axis. A fit to the baryon magnetic moments, constrained by the measured values of the axial vector coupling constants a(3)=F+Da^{(3)}=F+D, a(8)=3F−Da^{(8)}=3F-D, yields ⟨Sz⟩=0.08±0.13\langle S_z \rangle = 0.08 \pm 0.13, ⟨Lz⟩=0.39±0.09\langle L_z \rangle = 0.39 \pm 0.09, where the error is a theoretical estimate. A second fit, under slightly different assumptions, gives ⟨Lz⟩=0.37±0.09\langle L_z \rangle = 0.37 \pm 0.09, with no constraint on ⟨Sz⟩\langle S_z \rangle. The model provides a consistent description of axial vector couplings, magnetic moments and the quark polarization ⟨Sz⟩\langle S_z \rangle measured in deep inelastic scattering. The fits suggest that a significant part of the angular momentum of the proton may reside in a collective rotation of the constituent quarks.Comment: 16 pages, 3 ps-figures, uses RevTeX. Abstract, Sec. II, III and IV have been expande

    Magnetic and axial vector form factors as probes of orbital angular momentum in the proton

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    We have recently examined the static properties of the baryon octet (magnetic moments and axial vector coupling constants) in a generalized quark model in which the angular momentum of a polarized nucleon is partly spin ⟨Sz⟩\langle S_z \rangle and partly orbital ⟨Lz⟩\langle L_z \rangle. The orbital momentum was represented by the rotation of a flux-tube connecting the three constituent quarks. The best fit is obtained with ⟨Sz⟩=0.08±0.15\langle S_z \rangle = 0.08\pm 0.15, ⟨Lz⟩=0.42±0.14\langle L_z \rangle = 0.42\pm 0.14. We now consider the consequences of this idea for the q2q^2-dependence of the magnetic and axial vector form factors. It is found that the isovector magnetic form factor GMisovec(q2)G_M^{\mathrm{isovec}}(q^2) differs in shape from the axial form factor FA(q2)F_A(q^2) by an amount that depends on the spatial distribution of orbital angular momentum. The model of a rigidly rotating flux-tube leads to a relation between the magnetic, axial vector and matter radii, ⟨r2⟩mag=fspin⟨r2⟩axial+52forb⟨r2⟩matt\langle r^2 \rangle_{\mathrm{mag}} = f_{\mathrm{spin}} \langle r^2 \rangle_{\mathrm{axial}} + \frac{5}{2} f_{\mathrm{orb}} \langle r^2 \rangle_{\mathrm{matt}}, where forb/fspin=13⟨Lz⟩/GAf_{\mathrm{orb}}/ f_{\mathrm{spin}} = \frac{1}{3}\langle L_z \rangle / G_A, fspin+forb=1f_{\mathrm{spin}} + f_{\mathrm{orb}} = 1. The shape of FA(q2)F_A(q^2) is found to be close to a dipole with MA=0.92±0.06M_A = 0.92\pm 0.06 GeV.Comment: 18 pages, 5 ps-figures, uses RevTe

    Violation of Time Reversal Invariance in the Decays K_L -> pi^+ pi^- gamma and K_L -> pi^+ pi^- e^+ e^-

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    The origin of the large CP-odd and T-odd asymmetry observed in the decay K_L -> pi^+ pi^- e^+ e^- is traced to the polarization properties of the photon in the decay K_L -> pi^+ pi^- gamma. The Stokes vector of the photon S = (S_1, S_2, S_3) is studied as a function of the photon energy and found to possess CP-violating components S_1 and S_2 which are sizeable over a large part of the phase space, despite being proportional to the epsilon parameter of the K_L wave function. The component S_2 is T-even and manifests itself as a circular polarization of the photon, while S_1 is T-odd and gives rise to the asymmetry observed in K_L -> pi^+ pi^- e^+ e^-. The latter is shown to survive in the ``hermitian'' limit in which all unitarity phases are absent, and represents a genuine example of time reversal symmetry breaking in a CPT invariant theory.Comment: 4 pages including 2 figure

    Energy correlation and asymmetry of secondary leptons in H→ttˉH\to t\bar t and H→W+W−H\to W^+W^-

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    We study the energy correlation of charged leptons produced in the decay of a heavy Higgs particle H→ttˉ→bl+νlbˉl−νˉlH\to t\bar t\to bl^+\nu_l\bar bl^-\bar{\nu}_l and H→W+W−→l+νll−νˉl.H\to W^+W^-\to l^+\nu_ll^-\bar{\nu}_l. The possible influence of CPCP--violation in the HttˉHt\bar t and HW+W−HW^+W^- vertices on the energy spectrum of the secondary leptons is analyzed. The energy distribution of the charged leptons in the decay H→W+W−→l+νll−νˉlH\to W^+W^-\to l^+\nu_ll^-\bar{\nu}_l is sensitive to the CPCP--parity of the Higgs particle and yields a simple criterion for distinguishing scalar Higgs from pseudoscalar Higgs.Comment: 12 pages, + 4 uuencoded figures. report PITHA 94/2

    Positronium Decay : Gauge Invariance and Analyticity

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    The construction of positronium decay amplitudes is handled through the use of dispersion relations. In this way, emphasis is put on basic QED principles: gauge invariance and soft-photon limits (analyticity). A firm grounding is given to the factorization approaches, and some ambiguities in the spin and energy structures of the positronium wavefunction are removed. Non-factorizable amplitudes are naturally introduced. Their dynamics is described, especially regarding the enforcement of gauge invariance and analyticity through delicate interferences. The important question of the completeness of the present theoretical predictions for the decay rates is then addressed. Indeed, some of those non-factorizable contributions are unaccounted for by NRQED analyses. However, it is shown that such new contributions are highly suppressed, being of order alpha^3. Finally, a particular effective form factor formalism is constructed for parapositronium, allowing a thorough analysis of binding energy effects and analyticity implementation.Comment: 34 pages, 13 figure

    The CP-violating asymmetry in \eta\to\pi^+ \pi^- e^+e^-

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    We study the CP-violating asymmetry {\cal A}_{\rm CP}, which arises, in \eta\to\pi^+\pi^- e^+e^-, from the angular correlation of the e^+ e^- and \pi^+\pi^- planes due to the interference between the magnetic and electric decay amplitudes. With the phenomenologically determined magnetic amplitude and branching ratio as input, the asymmetry, induced by the electric bremsstrahlung amplitude through the CP-violating decay \eta\to\pi^+\pi^-, and by an unconventional tensor type operator, has been estimated respectively. The upper bound of {\cal A}_{\rm CP} from the former is about 10^{-3}, and the asymmetry from the latter might be up to O(10^{-2}). One can therefore expect that this CP asymmetry would be an interesting CP-violating observable for the future precise measurements in the \eta factories.Comment: LaTeX, 6 pages. One reference corrected, and some new references adde

    Charge asymmetries of top quarks: a window to new physics at hadron colliders

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    With the next start of LHC, a huge production of top quarks is expected. There are several models that predict the existence of heavy colored resonances decaying to top quarks in the TeV energy range. A peak in the differential cross section could reveal the existence of such a resonance, but this is experimentally challenging, because it requires selecting data samples where top and antitop quarks are highly boosted. Nonetheless, the production of such resonances might generate a sizable charge asymmetry of top versus antitop quarks. We consider a toy model with general flavour independent couplings of the resonance to quarks, of both vector and axial-vector kind. The charge asymmetry turns out to be a more powerful observable to detect new physics than the differential cross section, because its highest statistical significance is achieved with data samples of top-antitop quark pairs of low invariant masses

    Sagnac Interferometer Enhanced Particle Tracking in Optical Tweezers

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    A setup is proposed to enhance tracking of very small particles, by using optical tweezers embedded within a Sagnac interferometer. The achievable signal-to-noise ratio is shown to be enhanced over that for a standard optical tweezers setup. The enhancement factor increases asymptotically as the interferometer visibility approaches 100%, but is capped at a maximum given by the ratio of the trapping field intensity to the detector saturation threshold. For an achievable visibility of 99%, the signal-to-noise ratio is enhanced by a factor of 200, and the minimum trackable particle size is 2.4 times smaller than without the interferometer

    Effects of Chromate and Chromate Conversion Coatings on Corrosion of Aluminum Alloy 2024-T3

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    Various effects of chromate conversion coatings (CCCs) and chromate in solution on the corrosion of AA2024-T3 and pure Al are studied in this work. Raman spectroscopy was used to investigate the nature of chromate in CCCs through a comparison with the spectra of known standards and artificial Cr(III)/Cr(VI) mixed oxides. Chromate was shown to be released from CCCs and to migrate to and protect a nearby, uncoated area in the artificial scratch cell. However, experiments investigating the effect of chromate in solution on anodic dissolution kinetics under potentiostatic control indicated that large chromate concentrations were needed to have an effect.This work was supported by Major H. DeLong at the United States Air Force Office of Scientific Research under contracts F49620-96-1-0479 and F49620-96-0042
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