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corresponds to a small fractionAtip/Veff. Comparable effective reaction rateKrePdandKreTip,KrePd KreTipis assumed. This is justified on the basis of the greatly enhanced ... as compared to Pd(111). Detailed studies of this system were performed by Kolb and coworkers and presented in a poster by Dr Kibler at this Discussion meeting (see List ...

archive.nstl.gov.cn

VEFF

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1Introduction

Veff​(μEW)\displaystyle V_{\mathrm{\mathrm{eff}}}(\mu_{\mathrm{EW}}) =\displaystyle= Veff​(μc)≃0,\displaystyle V_{\mathrm{eff}}(\mu_{c})\simeq 0, (1) d​Veff​(μEW)d​μ\displaystyle\ \frac{dV_{\mathrm{eff}}(\mu_{\mathrm{EW}})}{d\mu} =\displaystyle= d​Veff​(μc)d​μ≃0\displaystyle\frac{dV_{\mathrm{eff}}(\mu_{c})}{d\mu}\simeq 0 (...

arxiv.org

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Realization of electroweak baryogenesis by fourth generation fermions

boson production via gluon fusion and to the Higgs decay into a photon pair were shown to be suppressed at least by a factor of10−210^{-2}compared with the top quark on... Veff​(0)=Veff​(ϕc)V_{\rm eff}(0)=V_{\rm eff}(\phi_{c}), at the critical temperatureT=TcT=T_{c}. The obtained ratioϕc/Tc≈0.9\phi_{c}/T_{c}\approx 0.9roughly meets the cri...

arxiv.org

Gravitational waveforms from periodic orbits around a Schwarzschild black hole embedded in a Dehnen-type dark matter halo

Veff=(1−2​Mr−32​π​ρs​rs3​r+rsrs2​r)​(1+L2r2),V_{\rm eff}=\left(1-\frac{2M}{r}-32\pi\rho_{s}r^{3}_{s}\sqrt{\frac{r+r_{s}}{r^{2}_{s}r}}\right)\left(1+\frac{L^{2}}{r^{2}}\right)\,, (8) whereVe​f​fV_{eff}is the effective potential for the motion of the test particle. To be more informative, we demonstrate the radial dependence of the effective poten...

arxiv.org

Signatures of Novikov–Thorne accretion disks around rotating black holes semiclassical gravity with trace anomaly

Veff=1−2​ℳer+L2−a2​(E2−1)r2−2​ℳe​(L−a​E)2r3.V_{\textrm{eff}}=1-\frac{2\mathcal{M}_{e}}{r}+\frac{L^{2}-a^{2}\left(E^{2}-1\right)}{r^{2}}-\frac{2\mathcal{M}_{e}\left(L-aE\right)^{2}}{r^{3}}. (13) For circular orbits, the radial velocity vanishes,r˙=0\dot{r}=0. Imposing the marginal stability conditions∂Veff/∂r=∂2Veff/∂r2=0\partial V_{\tex...

arxiv.org

Spectral instability modified Pöschl-Teller effective potential triggered by deterministic random perturbations

Veff=VPT+Vpert,\displaystyle V_{\mathrm{eff}}=V_{\mathrm{PT}}+V_{\mathrm{pert}}, (9) where we assume the parametersV0=b=5V_{0}=b=5for the Pöschl-Teller potential ... where one assumesV0=b=5V_{0}=b=5andϵ=0.001\epsilon=0.001. From left to right and top to bottom, we compare in pairs the resulting QNM spectra for different metric pe...

arxiv.org
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