Showing 521 - 540 results of 554 for search '"LL.M."', query time: 0.21s Refine Results
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    Single field inflation in the light of Pulsar Timing Array Data: quintessential interpretation of blue tilted tensor spectrum through Non-Bunch Davies initial condition by Sayantan Choudhury

    Published 2024-03-01
    “…Further, we compute a new field excursion formula using the Non-Bunch Davies initial condition, that validates the requirement of Effective Field Theory in the sub-Planckian regime, $$|\Delta \phi |\ll M_{\textrm{pl}}$$ | Δ ϕ | ≪ M pl for the allowed value of the tensor-to-scalar ratio, $$r<0.06$$ r < 0.06 from CMB observations. …”
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  5. 525

    The relationship between myofiber characteristics and meat quality of Chinese Qinchuan and Luxi cattle by Xiao Lu, Yuying Yang, Yimin Zhang, Yanwei Mao, Rongrong Liang, Lixian Zhu, Xin Luo

    Published 2021-04-01
    “…Objective The objectives of this study were to explore the expression patterns of myosin heavy chain (MyHC) genes of different skeletal muscles from Chinese cattle, and to investigate the relationship between myofiber characteristics and meat quality of M. longissimus lumborum (LL), M. psoas major (PM), and M. semimembranosus (SM) from Chinese Luxi and Qinchuan cattle. …”
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    The Makings of a Good Law School? by Michael Trebilcock

    Published 1991-01-01
    “…On moving to the University of Adelaide Law School in 1963, as a tutor while simultaneously undertaking an LL M by thesis, I encountered a law school which initially had six or seven full-time members of staff, with a great deal of practitioner instruction and much part-time study by students. …”
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  7. 527

    A new class of multiple nonlocal problems with two parameters and variable-order fractional p(⋅)-Laplacian by Mohamed Karim Hamdani, Lamine Mbarki, Mostafa Allaoui

    Published 2023-09-01
    “…The problem is stated as follows:</p> <p class="disp_formula"> $ \begin{eqnarray*} \left\{ \begin{array}{ll} M\Big(\sigma_{p(x, y)}(u)\Big)(-\Delta)^{s(\cdot)}_{p(\cdot)}u(x) = \lambda |u|^{q(x)-2}u\left(\int_{\Omega}\frac{1}{q(x)} |u|^{q(x)}dx \right)^{k_1}+\beta|u|^{r(x)-2}u\left(\int_{\Omega}\frac{1}{r(x)} |u|^{r(x)}dx \right)^{k_2} \quad \mbox{in }\Omega, \\ \ u = 0 \quad \mbox{on }\partial\Omega, \end{array} \right. …”
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  8. 528

    Inflation, proton decay, and Higgs-portal dark matter in $$SO(10) \times U(1)_\psi $$ SO(10)×U(1)ψ by Nobuchika Okada, Digesh Raut, Qaisar Shafi

    Published 2019-12-01
    “…The extra fermions acquire their masses from $$U(1)_\psi $$ U(1)ψ symmetry breaking, and a $$U(1)_\psi $$ U(1)ψ Higgs field drives a successful inflection-point inflation with a low Hubble parameter during inflation, $$H_{inf} \ll M_{I}$$ Hinf≪MI . Hence, cosmologically dangerous monopoles produced from SO(10) and PS breakings are diluted away. …”
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    On the planar Kirchhoff-type problem involving supercritical exponential growth by Zhang Limin, Tang Xianhua, Chen Peng

    Published 2022-05-01
    “…This article is concerned with the following nonlinear supercritical elliptic problem: −M(‖∇u‖22)Δu=f(x,u),inB1(0),u=0,on∂B1(0),\left\{\begin{array}{ll}-M(\Vert \nabla u{\Vert }_{2}^{2})\Delta u=f\left(x,u),& \hspace{0.1em}\text{in}\hspace{0.1em}\hspace{0.33em}{B}_{1}\left(0),\\ u=0,& \hspace{0.1em}\text{on}\hspace{0.1em}\hspace{0.33em}\partial {B}_{1}\left(0),\end{array}\right. where B1(0){B}_{1}\left(0) is the unit ball in R2{{\mathbb{R}}}^{2}, M:R+→R+M:{{\mathbb{R}}}^{+}\to {{\mathbb{R}}}^{+} is a Kirchhoff function, and f(x,t)f\left(x,t) has supercritical exponential growth on tt, which behaves as exp[(β0+∣x∣α)t2]\exp {[}({\beta }_{0}+| x\hspace{-0.25em}{| }^{\alpha }){t}^{2}] and exp(β0t2+∣x∣α)\exp ({\beta }_{0}{t}^{2+| x{| }^{\alpha }}) with β0{\beta }_{0}, α>0\alpha \gt 0. …”
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