The Murrell-Sorbie function of the ground state X 3Σ - g for sulfur molecule S 2 has been calculated by spectroscopic data and QCISD(T)/6-311 G ** method, respectively, which are in agreement in repulsive branch, however, there is a shallow maximum in attractive branch. This may be ...
We use essential cookies to make sure the site can function. We also use optional cookies for advertising, personalisation of content, usage analysis, and social media. By accepting optional cookies, you consent to the processing of your personal data - including transfers to third parties. Some...
We use essential cookies to make sure the site can function. We also use optional cookies for advertising, personalisation of content, usage analysis, and social media. By accepting optional cookies, you consent to the processing of your personal data - including transfers to third parties. Some...
scattering diffraction experiments carried out on a Sb(111) sample.He-Sb(111) bound states extracted fit to eight interaction potentials.An elastic close-coupling approach used to calculate the diffraction intensities.A corrugation height of 14 to 17 % of the lattice constant was derived.Calc. dif...
is a smooth function of two variables. The optimal eigenvalue type of these maps is found using a sequence space characterization of Besov-spaces due to Ciesielski-Figiel and sequence space estimates for "Besov-matrices" (of 5.4.). ... A Pietsch - Cambridge University Press 被引量: 812发表...
The HOMA-IR formula is based on a mathematical model of the insulin signaling pathway and, therefore, may not be suitable for lean populations, such as Asians, as well as those with lower beta-cell function and insulin secretion defects [29]. Furthermore, in the female subgroup, HOMA-IR ...
{\n background: #f2f2f2;\n margin: 0 auto;\n max-width: calc(1600px + 10%);\n padding: 30px 5% 16px;\n &:before,\n &:after {\n content: ' ';\n display: table;\n }\n &:after {\n clear: both;\n }\n a.c-uhff-ccpa {\n font-size: 11px;\n line-height: 16...
CalcUVBG |= planned_sync->calc_uvbg; WritePlane |= planned_sync->write_plane; } RandTable rnd = {0}; @@ -672,6 +676,7 @@ run(const int RestartSnapNum, const inttime_t ti_init, const struct header_data if(is_PM) { /* the if here is unnecessary but to signify checkpointing...
where the energy function \(f=f(x,\xi ):\omega \times {\mathbb {r}}^{n\times n}\rightarrow {\mathbb {r}}\) is quasiconvex with respect to \(\xi \) . one of the simplest examples considered by ball is given by functions f of the type $$\begin{aligned} f(\xi )=g(\xi...
whereN≥3,0<μ<N,α≥0and2α+μ<min{N+22,4}andGis the primitive of functiong. The potentialV:RN→Rmay decay to zero at infinity. By using variational methods, penalization technique andL∞-estimates, we obtain the existence of a positive solution for the above quasilinear Schrödinger...