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1 heta oscillations with a fixed amplitude and phase velocity.
2 n polariton mode with antiparallel group and phase velocities.
3 ements support the existence of two distinct phase velocities.
4  to larger presaccadic and postsaccadic slow-phase velocities.
5 ases occurred in the presence of higher slow-phase velocities.
6                                       The MR phase velocities (154 +/- 0.53 cm/s) compared favorably
7 nd ferromagnetic layers with modified photon phase velocities and magnon eigenfrequencies.
8                                Latency, slow phase velocity and asymmetry of the OOR were measured fr
9 llustrate these effects quantitatively, with phase velocity and attenuation variations changes under
10 tions affecting the charge distribution, SAW phase velocity and attenuation.
11                        The joint analysis of phase velocity and autospectrum gradient allowed the ide
12 o overcome this limitation through their low phase velocity and high field confinement.
13 ual feedback generally reduced the mean slow-phase velocity and the number of fast phases.
14 hese updated thermoelasticity data for these phases, velocity and density profiles for a pyrolite mod
15 version of receiver functions, Rayleigh-wave phase velocities, and modeling of the radial component o
16 ating group velocity and frequency-dependent phase velocities as novel biomarkers for plaque vulnerab
17  waves with a group velocity antiparallel to phase velocity, as observed experimentally.
18 from the cochlear base, where traveling-wave phase velocity attains a local minimum and a local maxim
19 ave type, we derive explicit expressions for phase velocity, attenuation coefficient, penetration dep
20  significant difference was observed in slow-phase velocities between the two assays (p = 0.40).
21                  This results in a different phase velocity between the collisionless zero sound and
22 frequency shift induced by the change in SAW phase velocity between the test group and control group,
23 amps or bumps, which perturb the LWFA bubble phase velocity by varying the plasma frequency and by af
24 that at the critical frequency the effective phase velocity changes discontinuously to a constant val
25 leration in the descending aorta measured by phase-velocity cine MRI (OR 1.68 for 100 mL/s(1.5) incre
26 of small molecules are carried out at mobile phase velocities close to (for isocratic runs) or somewh
27 ype VI showed significantly higher group and phase velocity compared to any other AHA type.
28 g ocean waves of similar frequency to a high phase velocity component at approximately double the fre
29                         In each subject, the phase-velocity data sets were used to generate dynamic v
30    There was reasonable agreement between MR phase velocity-derived PR fraction and that obtained fro
31 zed Bayesian inversion of Rayleigh group and phase velocity dispersions to estimate the lateral varia
32 The effect of the undulations of the carrier phase velocity due to large scale vortical structures an
33 so that there was a general decrease in slow-phase velocity gain with increasing temporal frequency.
34 se waves have a 300-kilometer wavelength and phase velocities greater than the local zonal flow by 10
35 re linear: column length vertical and mobile phase velocity horizontal.
36                                              Phase velocities in the control group ranged from 20 to
37 lumns were designed to have identical mobile-phase velocity in all channels in an effort to minimize
38 ght with an increase of around 15% in mobile phase velocity in nonretained measurements of Coumarin 4
39               The requirement of sub-luminal phase-velocity in laser-driven particle acceleration sch
40  measure the effect of compression on mobile-phase velocity, ionic sample fronts were monitored using
41 ation of terahertz radiation with subluminal phase velocities is a key issue in laser-driven particle
42 es as a function of column length and mobile phase velocity is a surface (z direction) to the x and y
43 ents could also be identified with group and phase velocity (lipid-rich necrotic core content, fibrou
44                             Multidimensional phase-velocity magnetic resonance imaging (PV-MRI) studi
45 e PR was measured by magnetic resonance (MR) phase velocity mapping and from real-time right ventricu
46 ce imaging (MRI) and magnetic resonance (MR) phase velocity mapping could provide accurate estimates
47            Magnetic resonance imaging and MR phase velocity mapping were then used to determine coarc
48 r pulmonary valvotomy, had PR measured by MR phase velocity mapping while breathing spontaneously.
49 irectly inferred from the signal phases, and phase velocity maps are obtained using Eikonal tomograph
50           We extract accurate dispersion and phase velocity maps of the cardiac waves and reveal vort
51                         Attenuation maps and phase-velocity maps are anti-correlated at periods betwe
52                     We conducted paired slow-phase velocity measurements in 5-day post-fertilization
53    Moreover, validation against experimental phase velocity measurements is also reported.
54 anks to their high field confinement and low phase velocity, motivating contemporary research to revi
55 ould provide a modification of the group and phase velocities of optical fields, raising the question
56                                          The phase velocities of Rayleigh waves increase more rapidly
57 nce occurs when charged particles exceed the phase velocity of a given medium.
58 ing air channel that modulates the effective phase velocity of a high-order waveguide mode.
59                        The model employs the phase velocity of acoustic-gravity waves that radiate du
60 rieto-occipital sites over the cortex with a phase velocity of approx. 8-14 m/s and wavelength of abo
61                              The sub-luminal phase velocity of electromagnetic waves in free space is
62  charged particle travelling faster than the phase velocity of light and a dielectric medium, such as
63 ckwaves of light when moving faster than the phase velocity of light in a medium.
64 ing through matter at speeds larger than the phase velocity of light in the medium emit Cherenkov rad
65 ticle moving with a velocity faster than the phase velocity of light in the medium radiates light tha
66 dium with a uniform velocity larger than the phase velocity of light in the same medium.
67 cities: the velocity of fluid transport, the phase velocity of metachronal waves, and the group veloc
68                                         Slow-phase velocity of MOKN and MSP were faster in response t
69 langiectasia in whom it seems to reduce slow-phase velocity of nystagmus.
70                                          The phase velocity of the wakefield of a laser wakefield acc
71                            By monitoring the phase velocity of the waveguide modes, we detect incoher
72  with group velocity and frequency-dependent phase velocity providing potentially complementary infor
73 ed as group velocity and frequency-dependent phase velocities, respectively, with results correlated
74 s an analyte band including pressure, mobile phase velocity, temperature, and retention factor.
75 nd to increase faster with increasing mobile phase velocity than the calculated values.
76 ed in resolving power by increases in mobile-phase velocity than the sub-2 microm porous silica packi
77 y fine particles are operated at high mobile phase velocities, the friction of the mobile phase perco
78                                     The slow-phase velocity, the quick-phase frequency, and the decay
79  factor (Q) characteristic and an ultra-high phase velocity up to 32395 ms(-1).
80 e modulation of horizontal and vergence slow phase velocity was greater at 0.5 Hz.
81 es faster than the surface plasmon polariton phase velocity, we can generate surface plasmon wakes, a
82                                     The slow phase velocities were higher in patients with FMN compar
83 t the observation of a change in the plasmon phase velocity when the excitation frequency approaches
84 ss in resolution from the increase in mobile phase velocity, which approximates an ideal, basic separ
85  By combining constraints from Rayleigh wave phase velocities with improved earthquake locations, we
86 e west than in the east, while the change in phase velocity with period is more uniform across the co