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 he nonlinear spectral changes induce by self-phase modulation.

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

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

5 was refined with a spatially dependent theta phase modulation.

6 hiral nematic reflector to achieve full 2pai phase modulation.

7 l zone responded exclusively to differential phase modulation.

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

9 trol with large antenna arrays, and flexible phase modulation.

10 asonically encode optical focusing with full-phase modulations.

11 ts exhibited a clear preference for encoding phase modulations.

12 phase-gradient metasurfaces that offer full-phase modulation (0 to 2pai) and high operation speeds r

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

14 ase precession of place cells, bidirectional phase modulation acted to return phaser cells to the sam

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

16 pproach that eliminates artifacts from cross-phase modulation and enables more rapid measurements by

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

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

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

20 ining data thanks to the intra-channel cross-phase modulation and intra-channel four-wave mixing trip

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

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

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

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

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

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

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

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

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

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

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

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

33 orted so far, however, still show incomplete phase modulation (below 360 ).

34 orted so far, however, still show incomplete phase modulation (below 360 degrees ).

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

36 Discrete Wavelet Transform (DWT) with random phase modulation, bilinear transformation, and nonlinear

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

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

39 smon resonances, with results showing a 3pai phase modulation capacity with a uniform reflection ampl

40 th intracavity-controlled Pancharatnam-Berry phase modulation, continuous and ergodic generation of s

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

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

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

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

45 surements are sometimes complicated by cross-phase modulation effects and dispersion of the broadband

46 on the order of ~ 1 fs from electronic self-phase modulation (ESPM).

47 (50-100 Hz) gamma power, as well as in theta phase modulation, even after controlling for the effects

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

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

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

51 Multifrequency phase/modulation fluorescence experiments qualitatively

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

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

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

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

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

57 k to infer the amplitude of the photothermal phase modulation from a short signal trace, trained in a

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

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

60 d of comb production uses electro-optic (EO) phase modulation in a resonator with strong second-order

61 They cause distinct phase modulations in momentum space, which directly refl

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

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

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

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

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

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

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

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

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

71 , we present a novel topologically protected phase modulation mechanism capable of achieving anti-sym

72 This new phase modulation mechanism expands the design toolbox of

73 cidate the underlying interfacial and cavity phase modulation mechanisms responsible for the dynamic

74 ave can be generated and influenced by cross-phase-modulation-mediated repetition-rate synchronizatio

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

76 20 kPa O2) in comparison with a conventional phase-modulation method based on a sinusoidally modulate

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

78 we demonstrate active color tuning based on phase modulation of a multilayer stack composed of a pha

79 locybin significantly decreased the level of phase modulation of cells with each neural frequency ban

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

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

82 two main alternatives are visually mediated phase modulation of neuronal oscillations (excitability

83 Beta phase modulation of phase-locked CA1 and PFC neurons dur

84 Controlled spectral phase modulation of the driver laser by means of an acou

85 space, which directly reflect the real-space phase modulation of the electronic transition density du

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

87 The separation was achieved by adjusting the phase modulation of the N(2)O exciting laser until a 90-

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

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

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

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

92 luate hiPSC-CM differentiation with: (1) two-phase modulation of Wnt, (2) dosage variant of GSK3beta

93 significant diel periodicity consistent with phased modulations of division observed in culture.

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

95 reported so far have achieved either limited phase modulation or low efficiency.

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

97 nal cord injury, albeit with preservation of phase modulation, probably affecting functional response

98 cortical locations and do so in part through phase-modulation rather than unstructured activation.

99 flex responses in forelimb muscles and their phase modulation remained largely unaffected after stagg

100 e and the supercontinuum (self seed) by self-phase modulation, resembling an "f-to-3f" interferometry

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

102 lence (23.5% of FSIs sampled) and magnitude (phase modulation strength: 22% of average response).

103 lenges by tuning its electronic structure of phase modulation synergistic with interfacial chemistry

104 By leveraging a dynamic phase modulation, the proposed linear phased array is no

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

106 Leveraging dynamic phase modulation, this concept holds immense promise for

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

108 f cameras at high resolution, (b) converting phase modulations to intensity modulations in the image,

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

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

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

112 By spatio-temporal spectral-phase-modulation, wave packets in the same or in differe

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

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

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

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

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

118 y neural populations contributing more to in-phase modulation, while inhibitory neural populations co

119 edented upper limit of 4pai range of dynamic phase modulation with no significant variations in optic

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