ライフサイエンスコーパス: standing wave

1 a pattern of light formed as a doughnut or a standing wave.

2 nce of a high frequency (500 kHz) ultrasonic standing wave.

3 In the orientation domain, it is a standing wave.

4 condensate in an amplitude-modulated optical standing wave.

5 , gentle particle manipulation by ultrasonic standing waves.

6 the pressure nodes or antinodes of acoustic standing waves.

7 oated particle-agglutination assays occur in standing waves.

8 ons from a travelling wave is probabilistic, standing wave absorption can be observed deterministical

9 Standing-wave ambient-pressure photoemission spectroscop

10 tates, the real-space distribution of phonon standing wave amplitudes, the scattering phase shifts, a

11 were located in the antinodes of an optical standing wave and were loaded from a Bose-Einstein conde

12 , this effect can be seen as the collapse of standing waves and transition to travelling waves within

13 , particle focusing using multinode acoustic standing waves, and a spatially arrayed detector, can in

14 In situ X-ray standing-wave atomic images relative to the hematite lat

15 honon-electron interactions in bulk acoustic standing wave (BAW) resonators made from piezoelectric s

16 e the incident and diffracted electric field standing wave becomes localized in regions of small CCA

17 monstrated via direct imaging of polaritonic standing waves by means of infrared nano-optics.

18 multiplanar excitation of fluorescence by a standing wave can be produced in a single-spot laser sca

19 This design makes optimum use of the standing wave cavity to improve the energy efficiency of

20 megahertz-frequency noncavitating ultrasonic standing waves concentrate at submillimetre distances an

21 digitated bar electrode array energized in a standing-wave configuration.

22 m chains along the direction of the acoustic standing wave due to radiation interaction forces exhibi

23 ptical traps is formed at the antinodes of a standing-wave evanescent field on a nanophotonic wavegui

24 ms are rare, but have been shown to resemble standing waves, except that they lack a characteristic w

25 e of dyes specific for the cell membrane how standing-wave excitation can be exploited to generate pr

26 Standing-wave excitation of fluorescence is highly desir

27 An acoustic standing wave field is generated in the microchannel, an

28 In an acoustic standing wave field the cells will be rotated until the

29 rmined by an applied high-amplitude acoustic standing wave field, in which particles move swiftly to

30 can only be acoustically levitated in simple standing-wave fields.

31 ces was investigated using long-period X-ray standing wave-florescence yield spectroscopy.

32 scence resonance energy transfer and optical standing wave fluorescence interferometry, we characteri

33 ed nuclei is investigated using a two-photon standing wave fluorescence photobleaching experiment wit

34 hickness in living cells (176 +/- 14 nm), by standing-wave fluorescence microscopy, and its F-actin d

35 absorber to control its interaction with the standing wave formed by the incident wave and its reflec

36 by exploring real-space profiles of plasmon standing waves formed between the tip of our nano-probe

37 We experimentally demonstrate that standing waves formed by two coherent counter-propagatin

38 be stably trapped in a surface plasmon (SP) standing wave generated by the constructive interference

39 familiar energy standing waves, polarization standing waves have constant electric and magnetic energ

40 ces coupled with the sensitivity provided by standing waves in an optical cavity and detection via im

41 an interaction of the cyclotron motion with standing waves in the trap cavity containing the electro

42 A liquid surface established by standing waves is used as a dynamically reconfigurable t

43 Here we employ a standing-wave laser field as a spatially resolving probe

44 s the near-field Talbot effect with a single standing-wave laser pulse as a phase grating.

45 Our work extends the domain of x-ray standing wave methods to resonant x-ray emission spectro

46 ervation that atoms could be diffracted by a standing wave of light.

47 f the pectoral and pelvic girdles creating a standing wave of the axial body.

48 n indicates the presence of a nodal line and standing waves on its surface.

49 ctures with a low laser power by combining a standing-wave optical trap with confocal Raman spectrosc

50 those in vivo and failed to recapitulate the standing wave oscillations observed in vivo.

51 in vivo dynamics of the Min system including standing wave oscillations.

52 n from the cytoplasm drives a self-organized standing wave oscillator.

53 Unlike current standing-wave parametric amplifiers, this traveling wave

54 the emergence of a distinct electromagnetic standing wave pattern in the cavity.

55 to avoid the formation of a nonphysiological standing wave pattern.

56 n conventional lasing systems, the resulting standing wave patterns exhibit only minimal overlap with

57 ser beams that create quasi-periodic optical standing-wave patterns.

58 In this method, we use standing-wave phase shifts to move particles or cells in

59 ressure X-ray photoelectron spectroscopy and standing-wave photoemission spectroscopy provides the sp

60 In contrast to familiar energy standing waves, polarization standing waves have constan

61 queous media by a combination of an acoustic standing wave pressure field and in situ complex coacerv

62 le argon atoms, traveling through an optical standing wave, produced a periodic array of localized me

63 phase can also be exploited to optimize the standing wave profile in planar devices to maximize ligh

64 pproaches such as coherent absorption from a standing wave promise total dissipation of energy.

65 Here, we present standing-wave Raman tweezers for stable trapping and sen

66 Evanescent standing wave (SW) illumination is used to generate a si

67 n normal visual responses, and both start as standing waves: synchronous elevated activity in the V1

68 sing an application of the long-period x-ray standing wave technique.

69 oustophoretic device that uses an ultrasonic standing wave to align the blood cells, which exhibit po

70 coustic flow cytometer that uses an acoustic standing wave to focus particles into 16 parallel analys

71 We report the first use of ultrasonic standing waves to achieve cell cycle phase synchronizati

72 hip for acoustophoresis utilizing ultrasonic standing waves to focus and orient red blood cells in tw

73 Here we use long-period x-ray standing waves to study the adsorption of mercurated-pol

74 tion wide-field biological imaging by use of standing wave total internal reflection fluorescence (SW

75 eaky waveguide (MCLW) sensor with ultrasound standing waves (USW).

76 characteristics of the accompanying electron standing waves, we are able to distinguish the fluorine

77 cident and diffracted waves, which creates a standing wave with nodes at strongly absorbing atoms.

78 reflected from a metallic mirror produces a standing wave with reduced intensity near the reflective

79 of pro-grade and retrograde flow rotations, standing waves with zero angular velocities can emerge.

80 terns appear stable, they are the product of standing waves, with auxin flowing through the tissue, m

81 Here, we use standing-wave X-ray fluorescence (SWXF) to localize chem

82 The variable-period x-ray standing wave (XSW) technique is emerging as a powerful