6,992 research outputs found

    PENGARUH MOTIVASI KERJA TERHADAP KINERJA KARYAWAN

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    The labor conditions in Indonesia are confronted with issues of unemployment, low productivity, and a significant number of workers employed in the informal sector. Low productivity impacts the level of employee performance. Performance becomes a crucial issue in the success of a company by requiring high-quality human resources. High-quality human resources will yield high performance. Enhancing performance requires motivation to create a greater sense of enthusiasm for task completion. The objective of this research is to determine the influence of work motivation on employee performance. This research employs a quantitative approach with data collected through accidental sampling technique involving 174 subjects. The analysis method used is multiple linear regression. The measurement tools used are IWPQ (Individual Work Performance Questionnaire) and MWMS (Multidimensional Work Motivation Scale), which consist of six dimensions: amotivation, extrinsic regulation social, extrinsic regulation material, introjected regulation, identified regulation, and intrinsic motivation. The overall results of this study through the six dimensions on the MWMS scale motivation does not have an influence on employee performance

    Constraining {\it CP} violation in a softly broken A4A_4 symmetric Model

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    To understand the mass spectra of charged lepton and neutrino A4A_4 symmetry has been proposed in addition with the Standard SU(2)L×U(1)YSU(2)_L\times U(1)_Y model. We break A4A_4 symmetry softly and the deviation from the tri-bimaximal mixing arises due to Zee mechanism. In the present work, we express two mixing angles θ13\theta_{13} and θ23\theta_{23} in terms of a single model parameter and experimental observables, such as, mixing angle θ12\theta_{12}, mass squared differences Δm212\Delta m^2_{21} and Δm322\Delta m^2_{32}. Using the experimental values of θ23\theta_{23}, θ12\theta_{12}, Δm212\Delta m^2_{21} and Δm322\Delta m^2_{32} we restrict the model parameter and we predict θ13\theta_{13}. This model gives rise to θ1311\theta_{13}\simeq 11^\circ if we allow 1σ1\sigma deviation of θ23\theta_{23} and 22^\circ deviation of θ12\theta_{12} from their best fit values. Utilizing all those constraints, we explore the extent of CP violation parameter JCPJ_{\rm CP} in the present model and found a value of JCP2.65×103J_{\rm CP}\approx 2.65\times 10^{-3} (for 1σ1\sigma deviation of θ23\theta_{23} and 22^\circ deviation of θ12\theta_{12}) consistent with the other neutrino experimental results. We have studied the mass pattern of neutrino and neutrinoless double beta decay (ββ0ν)(\beta\beta_{0\nu}) parameter (Mν)ee|(M_\nu)_{ee}| in this model.Comment: 16 pages, 6 eps figures,revised materials and figures, version to appear in Phys.Rev.

    Jet Identification with Zest

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    We present a new observable zest and demonstrate its potential to differentiate between jets originated by gluons, top quark and vector bosons. Zest has salient properties such as boost invariance, stability against global color flow of partons and inclusion or exclusion of a few soft particles to the jet. For a gluon jet, zest distribution is also insensitive to the jet mass. We show that when zest is used in conjunction with other observables, it can yield high gluon rejection while retaining high signal sample.Comment: 3 pages, 5 figures, XXII DAE-BRNS Symposium Proceeding

    Generalized Z2×Z2\mathbb{Z}_2\times \mathbb{Z}_2 in Scaling neutrino Majorana mass matrix and baryogenesis via flavored leptogenesis

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    We investigate the consequences of a generalized Z2×Z2\mathbb{Z}_2\times\mathbb{Z}_2 symmetry on a scaling neutrino Majorana mass matrix. It enables us to determine definite analytical relations between the mixing angles θ12\theta_{12} and θ13\theta_{13}, maximal CP violation for the Dirac type and vanishing for the Majorana type. Beside the other testable predictions on the low energy neutrino parameters such as ββ0ν\beta\beta_{0\nu} decay matrix element Mee|M_{ee}| and the light neutrino masses m1,2,3m_{1,2,3}, the model also has intriguing consequences from the perspective of leptogenesis. With the assumption that the required CP violation for leptogenesis is created by the decay of lightest (N1N_1) of the heavy Majorana neutrinos, only τ\tau-flavored leptogenesis scenario is found to be allowed in this model. For a normal (inverted) ordering of light neutrino masses, θ23\theta_{23} is found be less (greater) than its maximal value, for the final baryon asymmetry YBY_B to be in the observed range. Besides, an upper and a lower bound on the mass of N1N_1 have also been estimated. Effect of the heavier neutrinos N2,3N_{2,3} on final YBY_B has been worked out subsequently. The predictions of this model will be tested in the experiments such as nEXO, LEGEND, GERDA-II, T2K, NOν\nuA, DUNE etc.Comment: 37 pages, 12 figures, 9 tables, version accepted for publication in JHE
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