1,879 research outputs found

    Neutron electric dipole moment with external electric field method in lattice QCD

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    We discuss a possibility that the Neutron Electric Dipole Moment (NEDM) can be calculated in lattice QCD simulations in the presence of the CP violating ξ\theta term. In this paper we measure the energy difference between spin-up and spin-down states of the neutron in the presence of an uniform and static external electric field. We first test this method in quenched QCD with the RG improved gauge action on a 163×3216^3\times 32 lattice at a−1≃a^{-1}\simeq 2 GeV, employing two different lattice fermion formulations, the domain-wall fermion and the clover fermion for quarks, at relatively heavy quark mass (mPS/mV≃0.85)(m_{PS}/m_V \simeq 0.85). We obtain non-zero values of NEDM from calculations with both fermion formulations. We next consider some systematic uncertainties of our method for NEDM, using 243×3224^3\times 32 lattice at the same lattice spacing only with the clover fermion. We finally investigate the quark mass dependence of NEDM and observe a non-vanishing behavior of NEDM toward the chiral limit. We interpret this behavior as a manifestation of the pathology in the quenched approximation.Comment: LaTeX2e, 51 pages, 43 figures, uses revtex4 and graphicx, References and comments added, typos corrected, accepted by PR

    Full QCD calculation of neutron electric dipole moment with the external electric field method

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    We have calculated the neutron electric dipole moment (NEDM) in the presence of the CP violating Ξ\theta term in lattice QCD with 2-flavor dynamical clover quarks, using the external electric field method. Accumulating a large number of statistics by the averages over 16 different source points and over forward and backward nucleon propagators, we have obtained non-zero signals of neutron and proton EDM beyond one standard deviation at each quark mass in full QCD. We have investigated the quark mass dependence of nucleon EDM in full QCD, and have found that nucleon EDM in full QCD does not decrease toward the chiral limit, as opposed to the theoretical expectation. We briefly discuss possible reasons for this behavior.Comment: 27 pages, 15 figures, 2 tables, reference added, tyops corrected, published versio

    Lattice study of vacuum polarization function and determination of strong coupling constant

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    We calculate the vacuum polarization functions on the lattice using the overlap fermion formulation.By matching the lattice data at large momentum scales with the perturbative expansion supplemented by Operator Product Expansion (OPE), we extract the strong coupling constant αs(ÎŒ)\alpha_s(\mu) in two-flavor QCD as ΛMS‟(2)\Lambda^{(2)}_{\overline{MS}} = 0.234(9)(−0+16)0.234(9)(^{+16}_{- 0}) GeV, where the errors are statistical and systematic, respectively. In addition, from the analysis of the difference between the vector and axial-vector channels, we obtain some of the four-quark condensates.Comment: 24 pages, 9 figures, enlarged version published in Phys. Rev.

    Neutron electric dipole moment from lattice QCD

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    We carry out a feasibility study for the lattice QCD calculation of the neutron electric dipole moment (NEDM) in the presence of the Ξ\theta term. We develop the strategy to obtain the nucleon EDM from the CP-odd electromagnetic form factor F3F_3 at small Ξ\theta, in which NEDM is given by lim⁥q2→0ΞF3(q2)/(2mN)\lim_{q^2\to 0}\theta F_3(q^2)/(2m_N) where qq is the momentum transfer and mNm_N is the nucleon mass. We first derive a formula which relates F3F_3, a matrix element of the electromagnetic current between nucleon states, with vacuum expectation values of nucleons and/or the current. In the expansion of Ξ\theta, the parity-odd part of the nucleon-current-nucleon three-point function contains contributions not only from the parity-odd form factors but also from the parity-even form factors multiplied by the parity-odd part of the nucleon two-point function, and therefore the latter contribution must be subtracted to extract F3F_3. We then perform an explicit lattice calculation employing the domain-wall quark action with the RG improved gauge action in quenched QCD at a−1≃2a^{-1}\simeq 2 GeV on a 163×32×1616^3\times 32\times 16 lattice. At the quark mass mfa=0.03m_f a =0.03, corresponding to mπ/mρ≃0.63m_\pi/m_\rho \simeq 0.63, we accumulate 730 configurations, which allow us to extract the parity-odd part in both two- and three-point functions. Employing two different Dirac Îł\gamma matrix projections, we show that a consistent value for F3F_3 cannot be obtained without the subtraction described above. We obtain F3(q2≃0.58GeV2)/(2mN)=F_3(q^2\simeq 0.58 \textrm{GeV}^2)/(2m_N) = −-0.024(5) e⋅e\cdotfm for the neutron and F3(q2≃0.58GeV2)/(2mN)=F_3(q^2\simeq 0.58 \textrm{GeV}^2)/(2m_N) = 0.021(6) e⋅e\cdotfm for the proton.Comment: LaTeX2e, 43 pages, 42 eps figures, uses revtex4 and graphicx, comments added and typos corrected, final version to appear in Phys. Rev.

    Rectangular Wilson Loops at Large N

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    This work is about pure Yang-Mills theory in four Euclidean dimensions with gauge group SU(N). We study rectangular smeared Wilson loops on the lattice at large N and relatively close to the large-N transition point in their eigenvalue density. We show that the string tension can be extracted from these loops but their dependence on shape differs from the asymptotic prediction of effective string theory.Comment: 47 pages, 21 figures, 8 table

    Hadron Structure on the Lattice

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    A few chosen nucleon properties are described from a lattice QCD perspective: the nucleon sigma term and the scalar strangeness in the nucleon; the vector form factors in the nucleon, including the vector strangeness contribution, as well as parity breaking effects like the anapole and electric dipole moment; and finally the axial and tensor charges of the nucleon. The status of the lattice calculations is presented and their potential impact on phenomenology is discussed.Comment: 17 pages, 9 figures; proceedings of the Conclusive Symposium of the Collaborative Research Center 443 "Many-body structure of strongly interacting systems", Mainz, February 23-25, 201

    QCD corrections to the electric dipole moment of the neutron in the MSSM

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    We consider the QCD corrections to the electric dipole moment of the neutron in the Minimal Supersymmetric Standard Model. We provide a master formula for the Wilson coefficients at the low energy scale including for the first time the mixing between the electric and chromoelectric operators and correcting widely used previous LO estimates. We show that, because of the mixing between the electric and chromoelectric operators, the neutralino contribution is always strongly suppressed. We find that, in general, the effect of the QCD corrections is to reduce the amount of CP violation generated at the high scale. We discuss the perturbative uncertainties of the LO computation, which are particularly large for the gluino-mediated contribution. This motivates our Next-to-Leading order analysis. We compute for the first time the order alpha_s corrections to the Wilson coefficients for the gluino contributions, and recompute the two-loop anomalous dimension for the dipole operators. We show that the large LO uncertainty disappears once NLO corrections are taken into account.Comment: 23 pages, 5 figures, added references, corrected typo

    QKZ equation with |q|=1 and correlation functions of the XXZ model in the gapless regime

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    An integral solution to the quantum Knizhnik-Zamolodchikov (qqKZ) equation with ∣q∣=1|q|=1 is presented. Upon specialization, it leads to a conjectural formula for correlation functions of the XXZ model in the gapless regime. The validity of this conjecture is verified in special cases, including the nearest neighbor correlator with an arbitrary coupling constant, and general correlators in the XXX and XY limits

    The relationship between multilingual raters’ language background and their perceptions of accentedness and comprehensibility of second language speech

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    The purpose of this case study is twofold: it (1) explores multilingual raters’ judgements regarding the accentedness and comprehensibility of second language speech and (2) examines how the raters’ language backgrounds influence their judgements. In this study, six multilingual Singaporean raters judged the accentedness and comprehensibility of 50 unfamiliar accented speech samples produced by Japanese learners of English with different proficiency levels. In order to investigate rater judgement, the rating scores were subjected to a multifaceted Rasch analysis. A questionnaire and an interview elicited the raters’ retrospective reports on their language backgrounds at three time points in their life (when they were 5, 11, and 21 years old). The results suggested that the raters’ language backgrounds, notably the proficiency balance between multiple languages in early childhood, are related to their rating judgement

    Collagen I–mediated up-regulation of N-cadherin requires cooperative signals from integrins and discoidin domain receptor 1

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    Tumor cells undergo epithelial-to-mesenchymal transition (EMT) to convert from a benign to a malignant phenotype. Our recent focus has been signaling pathways that promote EMT in response to collagen. We have shown that human pancreatic cancer cells respond to collagen by up-regulating N-cadherin, which promotes tumor growth, invasion, and metastasis. Initial characterization showed that knocking down c-Jun NH2-terminal kinase prevented N-cadherin up-regulation and limited tumor growth and invasion in a mouse model for pancreatic cancer. The current study was designed to understand the pathway from collagen to N-cadherin up-regulation. Initiation of the signal requires two collagen receptors, α2ÎČ1 integrin and discoidin domain receptor (DDR) 1. Each receptor propagates signals through separate pathways that converge to up-regulate N-cadherin. Focal adhesion kinase (FAK)–related protein tyrosine kinase (Pyk2) is downstream of DDR1, whereas FAK is downstream of α2ÎČ1 integrin. Both receptor complexes rely on the p130 Crk-associated substrate scaffold. Interestingly, Rap1, but not Rho family guanosine triphosphatases, is required for the response to collagen I
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