ライフサイエンスコーパス: phase velocity

1 n polariton mode with antiparallel group and phase velocities.

2 ements support the existence of two distinct phase velocities.

3 to larger presaccadic and postsaccadic slow-phase velocities.

4 ases occurred in the presence of higher slow-phase velocities.

5 The MR phase velocities (154 +/- 0.53 cm/s) compared favorably

6 Latency, slow phase velocity and asymmetry of the OOR were measured fr

7 o overcome this limitation through their low phase velocity and high field confinement.

8 ual feedback generally reduced the mean slow-phase velocity and the number of fast phases.

9 hese updated thermoelasticity data for these phases, velocity and density profiles for a pyrolite mod

10 version of receiver functions, Rayleigh-wave phase velocities, and modeling of the radial component o

11 waves with a group velocity antiparallel to phase velocity, as observed experimentally.

12 from the cochlear base, where traveling-wave phase velocity attains a local minimum and a local maxim

13 leration in the descending aorta measured by phase-velocity cine MRI (OR 1.68 for 100 mL/s(1.5) incre

14 of small molecules are carried out at mobile phase velocities close to (for isocratic runs) or somewh

15 g ocean waves of similar frequency to a high phase velocity component at approximately double the fre

16 In each subject, the phase-velocity data sets were used to generate dynamic v

17 There was reasonable agreement between MR phase velocity-derived PR fraction and that obtained fro

18 so that there was a general decrease in slow-phase velocity gain with increasing temporal frequency.

19 se waves have a 300-kilometer wavelength and phase velocities greater than the local zonal flow by 10

20 re linear: column length vertical and mobile phase velocity horizontal.

21 Phase velocities in the control group ranged from 20 to

22 lumns were designed to have identical mobile-phase velocity in all channels in an effort to minimize

23 ght with an increase of around 15% in mobile phase velocity in nonretained measurements of Coumarin 4

24 The requirement of sub-luminal phase-velocity in laser-driven particle acceleration sch

25 measure the effect of compression on mobile-phase velocity, ionic sample fronts were monitored using

26 ation of terahertz radiation with subluminal phase velocities is a key issue in laser-driven particle

27 es as a function of column length and mobile phase velocity is a surface (z direction) to the x and y

28 Multidimensional phase-velocity magnetic resonance imaging (PV-MRI) studi

29 e PR was measured by magnetic resonance (MR) phase velocity mapping and from real-time right ventricu

30 ce imaging (MRI) and magnetic resonance (MR) phase velocity mapping could provide accurate estimates

31 Magnetic resonance imaging and MR phase velocity mapping were then used to determine coarc

32 r pulmonary valvotomy, had PR measured by MR phase velocity mapping while breathing spontaneously.

33 anks to their high field confinement and low phase velocity, motivating contemporary research to revi

34 The phase velocities of Rayleigh waves increase more rapidly

35 ing air channel that modulates the effective phase velocity of a high-order waveguide mode.

36 The sub-luminal phase velocity of electromagnetic waves in free space is

37 charged particle travelling faster than the phase velocity of light and a dielectric medium, such as

38 ckwaves of light when moving faster than the phase velocity of light in a medium.

39 ing through matter at speeds larger than the phase velocity of light in the medium emit Cherenkov rad

40 ticle moving with a velocity faster than the phase velocity of light in the medium radiates light tha

41 dium with a uniform velocity larger than the phase velocity of light in the same medium.

42 Slow-phase velocity of MOKN and MSP were faster in response t

43 langiectasia in whom it seems to reduce slow-phase velocity of nystagmus.

44 nd to increase faster with increasing mobile phase velocity than the calculated values.

45 ed in resolving power by increases in mobile-phase velocity than the sub-2 microm porous silica packi

46 y fine particles are operated at high mobile phase velocities, the friction of the mobile phase perco

47 factor (Q) characteristic and an ultra-high phase velocity up to 32395 ms(-1).

48 e modulation of horizontal and vergence slow phase velocity was greater at 0.5 Hz.

49 es faster than the surface plasmon polariton phase velocity, we can generate surface plasmon wakes, a

50 By combining constraints from Rayleigh wave phase velocities with improved earthquake locations, we