ライフサイエンスコーパス: phase modulation

1 d relative modulation (i.e., the strength of phase modulation).

2 e-level amplitude modulation and eight-level phase modulation.

3 anomalous group-velocity dispersion and self-phase modulation.

4 was refined with a spatially dependent theta phase modulation.

5 l zone responded exclusively to differential phase modulation.

6 ase-sensitive neurons in the ELL to a common phase modulation.

7 ts exhibited a clear preference for encoding phase modulations.

8 Phase-modulation 2D fluorescence spectroscopy (PM-2D FS)

9 ) catalysis-defective mutant is normal for S-phase modulation and DSB-independent homolog pairing but

10 -division-multiplexing channels, large cross-phase modulation and four-wave mixing crosstalks among t

11 ntal reasons, is always accompanied by cross-phase modulation and four-wave mixing.

12 quantization is realized by the strong cross-phase modulation and interference in a silicon-organic h

13 ction of the propagating optical field (self-phase modulation and modulation instability).

14 s that require external/pumping waves (cross-phase modulation and parametric processes such as four-w

15 s in the literature, while no time-consuming phase modulation and phase extraction processes are requ

16 tion by RB50 does not require Bvg phenotypic phase modulation and that isogenic Bvg(Con) and Bvg(-) p

17 feature is achieved by leveraging the local phase modulation and the non-local lattice diffraction v

18 pulses with adjustable amplitude using only phase modulation and the nonlinear response of a medium.

19 quency modulation, amplitude modulation, and phase modulation are all observed.

20 gnals, amplitude modulation and differential phase modulation, are essential for an African wave-type

21 y in tissue-like scattering, measurements of phase modulation as a function of modulation frequency w

22 ich results in a transmitted electromagnetic phase modulation as large as 0.56pi.

23 improved sensitivity and dynamic control for phase modulation, as we believe can be enabled by piezoe

24 Here, we propose a method to realize phase modulation at subwavelength length scales while ma

25 re, we demonstrate a large conditional cross-phase modulation between a signal field, stored inside a

26 derlying mechanism is based on an asymmetric phase modulation by coupling a phase array and a near-ze

27 Spiking activity demonstrated consistent phase modulation by ongoing brain oscillations and was s

28 that while all kinetic models could describe phase-modulation data in nonscattering solution, when in

29 inetic parameters failed to likewise predict phase-modulation data in scattering solutions.

30 The long lifetime of RuCon A allows phase-modulation decay time measurements using an amplit

31 ial application of BP in ultrafast nonlinear phase modulation devices based on their nonlinear optica

32 Using self - phase modulation experiments, we characterize a waveguid

33 By applying a phase-modulation fluorescence approach to 2D electronic

34 esolved fluorescence quenching, differential phase/modulation fluorescence anisotropy, and 1H NMR stu

35 Multifrequency phase/modulation fluorescence experiments qualitatively

36 and absence of calcium, using multifrequency phase-modulation fluorimetry.

37 glucose/galactose binding protein (GGBP) and phase-modulation fluorometry.

38 cellular free sodium using frequency-domain, phase-modulation fluorometry.

39 interaural phase difference (the interaural phase modulation following response; IPM-FR).

40 osin subfragment 1 (S1) using multifrequency phase/modulation Forster resonance energy transfer (FRET

41 tasurfaces, we demonstrate a novel amplitude-phase modulation hologram with simultaneous five-level a

42 g by nonlinear spectral broadening from self-phase modulation in a nanowire waveguide, followed by te

43 e second type are created by dual-pump cross-phase-modulation-induced FWM sideband generation and can

44 ized guinea pigs were recorded to interaural phase modulation (IPM) before, during, and after iontoph

45 y-managed nonlinear medium where strong self-phase modulation is achieved without nonlinear inter-cha

46 y-managed nonlinear medium where strong self-phase modulation is achieved without such nonlinear cros

47 This large phase modulation is afforded in the cost of low transmis

48 nd to match those measured using traditional phase-modulation measurement in nonscattering media.

49 iological samples during frequency domain or phase modulation measurements of intensity decays.

50 ttribute the results to the insensitivity of phase-modulation measurements in nonscattering solutions

51 Our results suggest the high sensitivity of phase-modulation measurements in scattering solutions ma

52 show that use of the proposed multifrequency phase-modulation method (1) provides adequate modeling o

53 20 kPa O2) in comparison with a conventional phase-modulation method based on a sinusoidally modulate

54 We propose a novel multifrequency phase-modulation method for luminescence spectroscopy th

55 z oscillation in the PFC and the VTA and its phase modulation of gamma power in both structures was p

56 ma frequency band and the magnitude of theta-phase modulation of gamma power were significantly decre

57 ne) can be enhanced by 15% through iterative phase modulation of the excitation pulse.

58 lactate is observed indirectly by monitoring phase modulation of the spin-coupled hyperpolarized (13)

59 we provide an experimental demonstration of phase modulation of THz beam by operating a ferroelectri

60 s monitored in real time using two-frequency phase modulation of tissue-embedded phosphorescent micro

61 ical oscillator to create dual combs through phase modulation of two optical signals that have a stab

62 st of the previous designs utilize the local phase modulation only and operate optimally for a specif

63 nstants are about 5- to 10-fold smaller with phase, modulation, or mean lifetime than with intensitie

64 We report the spatial self-phase modulation (SSPM) effect for solution dispersions

65 responded to both amplitude and differential phase modulation, they did not differentiate between tem

66 eometries, we demonstrate the use of dynamic phase modulation to grow symmetric crystal junctions wit

67 ompression/reflection pattern provides a two-phase modulation: V1 is first depolarized by the primary

68 oduced a small but significant change in our phase/modulation versus frequency data, showing that cha

69 Spatially random phase modulation was implemented for the lower speckle i

70 have unique features, such as, amplitude and phase modulation waves and also exhibited formation of s

71 Based on cross phase modulation, we present an approach to realizing a

72 aveguide that can produce high-speed optical phase modulation: we demonstrate an all-silicon optical

73 of negative fourth-order dispersion and self-phase modulation, which can occur even for normal group-

74 uires strong optical nonlinearity, e.g. self-phase modulation, which, for fundamental reasons, is alw

75 Wavelengths (ZDWs) and the process of cross phase modulation with soliton fission, red-shifted dispe