The rs value has a strong dependence on carrier concentration with the relationship given as 4 3 pa3B rs3~n3d in 3D case32. Here, aB5(e/mb)ab 5 1.54 nm, which gives the effective Bohr radius with dielectric constant of e58.45 and effective mass of conduction-band electron (mb50.29me...
However, the p-wave topological superfluid of ultracold atoms is either collisionally unstable near a Feshbach resonance, or has a vanishingly low superfluid transition temperature far from the resonance22–24. Successful experiments on the creation of ground-state ultracold polar molecules25–36 ...
“The North and South Poles are not melting.” In that report, oceanographer Ted Maksym noted that polar ice “is much more stable than climate scientists once predicted and could even be much thicker than previously thought.” That Woods Hole study was confirmed by today’s NOAA Arctic radar...
Express 8, 113002 (2015). 30. Hirai, T. et al. Control of magnetic anisotropy in Pt/Co system using ionic liquid gating. Appl. Phys. Express 9, 063007 (2016). 31. Carcia, P. F. Perpendicular magnetic anisotropy in Pd/Co and Pt/Co thin-film layered structures. J. Appl. Phys. 63...
(see Supplementary Note2for details). The electric field induces the site energy difference in each dimer. This change gives rise to the charge disproportionation along the electric-field direction (Fig.3dand Fig.4a, b) and also increases the splitting of the bonding and anti-bonding orbitals,...
Like point clouds representing the surface of a 3D entity, large quantities of dynamic particles express physical phenomena effectively. By rendering massive unevenly distributed and animated particles, dynamic cyclone activities will be simulated and tracked from birth to death with the wind simulation ...
It is customary to express 𝐹∞𝐸FE∞ as: 𝐹∞𝐸=𝑅2𝐷2𝐻∞𝐸,FE∞=R2D2HE∞, (1) where 𝐻∞𝐸HE∞ is the effective flux, that is formally independent of D. It can be calculated as an integral of the radiating surface flux over the visible part of the surface, ...