Showing 2,721 - 2,740 results of 3,537 for search 'Luptin~', query time: 1.86s Refine Results
  1. 2721

    Speech Act Use in Jokowi Political Communication during The Press Conference of The State Visit in Moskow by Gabriel Fredi Daar, Fransiskus Jemadi

    Published 2023-06-01
    “…The data were analyzed using Austin's speech act theory (1962) and Searle's (1979). …”
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    Ficolins and the Recognition of Pathogenic Microorganisms: An Overview of the Innate Immune Response and Contribution of Single Nucleotide Polymorphisms by Stefan Bidula, Darren W. Sexton, Silke Schelenz

    Published 2019-01-01
    “…Pathogens are primarily removed by direct opsonisation following the recognition of cell surface carbohydrates and other immunostimulatory molecules or via the activation of the lectin complement pathway, which results in the deposition of C3b and the recruitment of phagocytes. …”
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  8. 2728
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    Higher precision constraints on the tau $$g-2$$ g - 2 in LHC photon-initiated production: a full account of hadron dissociation and soft survival effects by L. A. Harland-Lang

    Published 2024-12-01
    “…Abstract We present the first calculation of photon-initiated $$\tau $$ τ pair production in the presence of non-zero anomalous magnetic ( $$a_\tau $$ a τ ) and/or electric dipole ( $$d_\tau $$ d τ ) moments of the $$\tau $$ τ lepton that accounts for the non-trivial interplay between these modifications with the soft survival factor and the possibility of dissociation of the hadron (proton or ion) beam. …”
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    Kinetics and Mechanism of Nickel(II) Ion Biosorption by Immobilized Brown Algae by Wen Hong Fan, Zhi Zhen Xu, Qian Li

    Published 2010-07-01
    “…The biosorption of Ni(II) ions by brown Laminaria japonica algae immobilized in sodium alginate and glutin beads was investigated. The kinetics of Ni(II) ion biosorption within the immobilized L. japonica beads were described well by the pseudo-second-order model. …”
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  12. 2732

    A biomechanical study of the role of sitagliptin on the bone characteristics of diabetic rats by Stavros K Kourkoulis, Ermioni Pasiou, Arezoo Abdi, Despoina Perrea, John Vlamis

    Published 2020-01-01
    “…Finally, it seems that treating diabetic animals with sita­gliptin only partly reverses the effect of Type 2 Diabetes Mellitus on their bone tissue, at least concerning its strength and stiffness.…”
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    Constraining the Effective Mass of Majorana Neutrino with Sterile Neutrino Mass for Inverted Ordering Spectrum by Jaydip Singh

    Published 2019-01-01
    “…This observation would allow establishing physics beyond the standard model and phenomena like lepton number violation and Majorana nature of neutrino. …”
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  15. 2735

    L’organisation comme effet de médiation : Redéfinir le lien entre organisation et communication by François Cooren, James R. Taylor

    Published 2024-02-01
    “…La théorie des actes de langage (Austin, Searle et Vanderveken) est mobilisée et reformulée selon un nouveau modèle analytique basé sur le concept de « modalité » emprunté à la théorie greimassienne et la théorie de la sémantique des modalités (Palmer, Bybee et Fleischman). …”
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    Scrutinizing $$B^0$$ B 0 -meson flavor changing neutral current decay into scalar $$K_0^*(1430)$$ K 0 ∗ ( 1430 ) meson with $$b\rightarrow s \ell ^+\ell ^-(\nu \bar{\nu })$$ b → s... by Yin-Long Yang, Ya-Xiong Wang, Hai-Bing Fu, Tao Zhong, Ya-Lin Song

    Published 2025-01-01
    “…Furthermore, we calculate the $$B^0\rightarrow K_0^*(1430)\ell ^+\ell ^-(\nu \bar{\nu })$$ B 0 → K 0 ∗ ( 1430 ) ℓ + ℓ - ( ν ν ¯ ) decay widths, branching fractions, and longitudinal lepton polarization asymmetries of $$B^0\rightarrow K_0^*(1430)\ell ^+\ell ^-$$ B 0 → K 0 ∗ ( 1430 ) ℓ + ℓ - , which lead to $$\mathcal{B}(B^0\rightarrow K_0^*(1430)e^+e^-) = (6.65^{+2.52}_{-2.42})\times 10^{-7}$$ B ( B 0 → K 0 ∗ ( 1430 ) e + e - ) = ( 6 . 65 - 2.42 + 2.52 ) × 10 - 7 , $$\mathcal{B}(B^0\rightarrow K_0^*(1430)\mu ^+\mu ^-)=(6.62^{+2.51}_{-2.41})\times 10^{-7}$$ B ( B 0 → K 0 ∗ ( 1430 ) μ + μ - ) = ( 6 . 62 - 2.41 + 2.51 ) × 10 - 7 , $$\mathcal{B}(B^0\rightarrow K_0^*(1430)\tau ^+\tau ^-)=(1.88^{+1.10}_{-0.97})\times 10^{-8}$$ B ( B 0 → K 0 ∗ ( 1430 ) τ + τ - ) = ( 1 . 88 - 0.97 + 1.10 ) × 10 - 8 , $$\mathcal{B}(B^0\rightarrow K_0^*(1430)\nu \bar{\nu })= 3.85^{+1.55}_{-1.48}\times 10^{-6}$$ B ( B 0 → K 0 ∗ ( 1430 ) ν ν ¯ ) = 3 . 85 - 1.48 + 1.55 × 10 - 6 and the integrated longitudinal lepton polarization asymmetries $$\langle A_{P_L} \rangle = (-0.99, -0.96, -0.03)$$ ⟨ A P L ⟩ = ( - 0.99 , - 0.96 , - 0.03 ) for the cases $$\ell =(e, \mu , \tau )$$ ℓ = ( e , μ , τ ) respectively.…”
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