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1 article illuminated by an obliquely incident plane wave.
2 originate from fine interference of multiple plane waves.
3 riance of the speed of light only applies to plane waves.
4 nsional stochastic model of random-direction plane waves.
5 smon modes that are difficult to excite with plane waves.
6 rom 25 to 800 THz) under normal incidence of plane waves.
7 non is theoretically explored by considering plane wave and Gaussian pulse propagation in an unbounde
8 oth near-field and far-field properties with plane wave and lumped port sources.
9            We present explicit solutions for plane waves and linear excitations, and identify the dif
10 ta-band activity is dominated by propagating plane waves and spatiotemporal structures, which we call
11                    This activity consists of plane waves and spiral-like waves, as well as more compl
12 red from long, thin objects illuminated by a plane wave at any angle.
13 NMR with first-principles calculations using plane-wave basis sets.
14        In perfect crystals, normal modes are plane waves, but they can be complex in disordered syste
15 me but lose both longitudinal and transverse plane-wave character at a common energy near the Boson p
16   An 18-MHz linear array was used to acquire plane-wave data at absolute frame rates >/=10 kHz using
17 of theory, including both Gaussian-based and plane wave density functional theory (DFT), second-order
18  spectroscopy (VT-DRIFTS) aided by ab initio plane wave density functional theory, that similar evide
19                        We present results of plane-wave density functional theory (DFT) based investi
20 as well as its surface mobility, by means of plane-wave density functional theory (DFT) calculations.
21          (1) J(OH) and D(OH) calculated from plane-wave density functional theory (DFT) show very goo
22                                  Employing a plane-wave density functional theory formalism, we inves
23                                              Plane-wave density functional theory has been applied in
24 P-dependent protein kinase are calculated by plane-wave density functional theory, starting from stru
25 a and phosphoric acid are investigated using plane-wave density functional theory.
26 (1)H-(17)O scalar and dipolar couplings, and plane-wave DFT calculations provide a method to precisel
27 large, uniform and surface-normal free-space plane waves directly from dispersion-engineered photonic
28 port, we evaluate the potential of ultrafast plane-wave Doppler ultrasound (PWU) to detect increased
29 ultiplex the hologram with multiple off-axis plane waves, duplicating the pupils into an array.
30 on of the mode-coupling coefficients for the plane wave expansion and the orthonormal fluctuation mod
31 electron full-potential linearized augmented plane wave (FLAPW) approach across various functionals f
32 with the full-potential linearized augmented plane wave (FLAPW) method show that the band gap increas
33 ds using full potential linearized augmented plane wave (FPLAPW) method under generalized gradient ap
34 bles the guided waves that are essentially a plane wave freely propagating along the in-plane, but co
35                                          The plane waves have an average phase gradient of approximat
36            The normal modes take the form of plane waves hybridized with localized short wavelength f
37 switchable with the polarization of uniform, plane wave illumination, and its magnitude is comparable
38  a 40[Formula: see text] objective lens with plane wave illumination.
39 ted for a quantitative analysis of SPR under plane-wave illumination and a finite-difference time-dom
40 st imaging and ptychography in conventional, plane-wave illumination TEM.
41 ame rate given the large number of elements, plane wave imaging was implemented with all three arrays
42                                      Here, a plane-wave imaging method was used to obtain high-speed
43 ch combines nonlinear pulsing sequences with plane-wave imaging to segment microbubble signals indepe
44                                   Compounded plane-wave imaging was used to acquire the ultrasound im
45 des more selective than circularly polarized plane waves in preferentially exciting single enantiomer
46 eous unit cells can turn a normally incident plane wave into a self-accelerating beam on the prescrib
47 le frequency sweep, compressing the incoming plane-waves into a single channel through the transfer f
48 space non-symmorphic symmetries and a kagome plane-wave lattice structure.
49       We send a perfect circularly-polarized plane-wave light onto plasmonic optical vortex generator
50 trogen transport occurs uniformly creating a plane-wave-like migration front, without assistance of d
51 ing STWPs typically relies on a continuum of plane-wave modes, their multimode-fiber counterparts mus
52 equilibrium Bose-Einstein distribution at in-plane wave number k parallel > 0 and a nonequilibrium co
53 erent radiation masks to encode the incoming plane waves on the radar aperture using a single channel
54 ndles relatively simple light beams, such as plane waves or Gaussian beams.
55 lly periodic firing patterns are composed of plane waves (or bands) drawn from a discrete set of orie
56 origin of displaying both wave property from plane wave part of the general Fourier expansion and par
57 transform operation applied to the retrieved plane-wave projection patterns.
58 iversity concept, spatial information of the plane-wave projections on the radar aperture is retrieve
59       The most familiar example is that of a plane wave propagating in free space.
60 , we obtained good agreement with theory for plane waves propagating in a direction perpendicular to
61                                              Plane waves propagating parallel to myocardial fibers pr
62 el to fibers (10.6 +/- 4.2 mm) compared with plane wave propagation (ie, without pivoting) parallel t
63 n be explained by a large decrease in the in-plane wave propagation length that occurs near the molec
64 ring reentry was compared with lambda during plane wave propagation transverse and longitudinal to ca
65 pic bidomain nature of cardiac tissue during plane wave propagation.
66 es chemical shift calculations that employ a plane-wave pseudopotential approach.
67 proach to hybridizing orbital (molecule) and plane-wave (semiconductor/material) systems to better de
68 lly incoherent radiation masks to encode the plane-wave signals incident on the radar aperture using
69 ping a spatially localized basis, compressed plane waves, that spans the eigenspace of a differential
70           The coupling of an electromagnetic plane wave to a thin conductor depends on the sheet cond
71      Our approach generalizes the concept of plane waves to an orthogonal real-space basis with multi
72 erfused with MB and sonicated with different plane-wave transmission patterns.
73 ce and that of the second mechanism is an in-plane wave vector matching when the Dirac points of the
74 r new wavelet formation after collision of a plane wave with an obstacle in an otherwise homogeneous
75 erically prove that under an electromagnetic plane wave with linear polarization incident normally to