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Currently simulations can be performed on large organic materials employing many body potentials for millions of atoms for times of many picoseconds.
They required that the two body potentials lie in (L^{nu /2+epsilon } cap L^{nu /2-epsilon }), but given Theorem 14.9, their method works for two body potentials in (L^{nu /2}). .
(Lavine [413, 414, 415, 416]) Let H be an N-body Hamiltonian with center of mass removed on (L^2({mathbb {R}}^{ N-1)nu })) whose two body potentials (V_{ N-1 lie inu(L^p({mathbb {R}}^nu )+L^infty ({mathbb {R}}^nu )) (whosep (nu )-canonical) and are repulsive.
Previous work and the current study mainly focus on atomic species with simple London dispersion interactions and simple many body potentials for metallic atoms system such as Ni.
There are many examples where bond valences have been used to analyze or confirm simulations obtained by two body potentials, density functional theory, or other quantum methods.
Figure 2 and B show the ECG recorded in lead I and the distribution of body potentials during the activation and the repolarization phase, recorded at 40 and 310 ms after the endocardial stimulation respectively.
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The empirical two body potential, originally designed for the liquid state, reproduces quite accurately our experimental results.
A detailed analysis of the body potential impact on the performance enhancement of Body Contacted (BC) pMOSFET when the body is not grounded, is reported in this paper.
Since the body is floating, the extra holes (for nMOSFETs) in this region accumulate, causing body potential arise, which of course degrades the performance of the device.
The interaction between atoms Cu Cu, Pd Pd as well as Cu Pd were calculated by Quantum Sutton Chen (Q SC) many body potential.
Static characterizations of various layouts and geometries demonstrate that narrow pMOSFET and H-gate design provides the highest Ion gain due to higher body potential.
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