equationin examining red/green color vision Methods: The reasons are explained – (1) for which Rayleigh spectral emissions deserve careful balancing with cone spectral absorbances, and – (2) for which defined field luminance, field diameter and neutral adaptation are decisive criteria for ...
Communications in Mathematical Physics Jia Shen, Avy Soffer& Yifei Wu 653Accesses 2Citations Explore all metrics Abstract We study the random data problem for 3D, defocusing, cubic nonlinear Schrödinger equation inHxs(R3)withs<12. First, we prove that the almost sure local well-posedness holds...
Compact and portable low-coherence interferometer with off-axis geometry for quantitative phase microscopy and nanoscopy Opt Express, 21 (5) (2013), pp. 5701-5714 View in ScopusGoogle Scholar [40] R.V. Shack Production and use of a lecticular hartmann screen J Opt Soc Am, 61 (1971), pp...
Not what you’re looking for? Submit your question to a subject-matter expert. Send to expertPrevious question Next question Transcribed image text: Use the RegionPlot3D command to drew a picture of a cone with its point at the region. The...
The aim of this article was to address the lump, lump-one stripe, multiwave and breather solutions for the Hunter–Saxton equation with the aid of Hirota bilinear technique. This model concerns in a massive nematic liquid crystal director field. By choosing the function f in Hirota bilinear for...
2. Some critical point theorems In this section, we recall some abstract critical point theorems we will apply in the proof of our main results. Throughout the section, X, · is a Hilbert space and P ⊂ X is a closed convex cone. For ε > 0, we denote by Vε(S) the ε-...
3D scattering problemcone-spherecylinderhemispherical capsA rigorous implementation, in an edge-based finite element formulation, of a second-order absorbing boundary condition (ABC) is presented for the solution of the 3-D scattering problem when the boundary S terminating the mesh is conformal to ...
The numerical model used in 3D calculations is shown in Figure 12; the OVITO program [90] was used for visualization with each SPH particle represented by a small sphere. The number of SPH particles was chosen from a preliminary parametric study to provide a compromise between the precision and...
The missing-cone problem in ODT is addressed by using the iterative non-negative constraint algorithm, and the misalignment of the LED array is further numerically corrected to improve the accuracy of refractive index quantification. Experiments on polystyrene beads and thick biological specimens show ...