ライフサイエンスコーパス: evanescent wave

1 tection on a liquid-solid interface based on evanescent wave.

2 ng refraction, total internal reflection and evanescent wave.

3 es the metal layer and illuminates muscle by evanescent wave.

4 the distance-dependent intensity decay of an evanescent wave.

5 g angle with the depth of penetration of the evanescent wave.

6 instead of diverging, because of the role of evanescent waves.

7 resolved images by restoring propagative and evanescent waves.

8 anescent-wave sensors to detect the mid-(IR) evanescent-wave absorbance spectra of small areas of bio

9 luorophore is monitored as a function of the evanescent wave absorption of an analyte-sensitive indic

10 TIRF-FOB are (i) fluorescence is excited via evanescent waves and amplified via liposomes; (ii) the u

11 gs illuminate the unusual transverse spin in evanescent waves and explain recent experiments that hav

12 This study reports a reusable evanescent wave aptamer-based biosensor for rapid, sensi

13 propagating waves are focused and, moreover, evanescent waves are reconstructed in the image plane.

14 Evanescent waves are ubiquitous at interfaces with optic

15 dy the lateral and vertical distributions of evanescent waves around the image plane of such a lens,

16 ial variations of the wave field (carried by evanescent waves), as the one created by edges or small

17 The depth of the evanescent wave at different layers was altered by tunin

18 ng analyte-containing medium by means of the evanescent wave at the fiber boundary.

19 paves the way for the establishment of novel evanescent wave-based systems.

20 The concentration detection limit of the MB evanescent wave biosensor is 1.1 nM.

21 zed in a polymer matrix, as detected with an evanescent wave biosensor, was investigated.

22 Evanescent wave biosensors have found a wide array appli

23 The application of evanescent wave cavity ring-down spectroscopy (EW-CRDS)

24 Evanescent wave cavity ringdown spectroscopy (EW-CRDS) i

25 sociation kinetics and diffusion through the evanescent wave contribute to the fluorescence fluctuati

26 sociation kinetics and diffusion through the evanescent wave contribute to the fluorescence fluctuati

27 ee orders of magnitude over the conventional evanescent-wave coupling.

28 offers important advantages over traditional evanescent-wave detection strategies which rely on recor

29 We have prepared a novel optical fiber evanescent wave DNA biosensor using a newly developed mo

30 Azimuthal beam scanning makes evanescent-wave (EW) excitation isotropic, thereby produ

31 duct of two near-field factors: the depth of evanescent wave excitation and a distance-dependent coup

32 ends on two near-field factors: the depth of evanescent wave excitation and a distance-dependent coup

33 liter with an automated array biosensor and evanescent wave excitation for fluorescence measurements

34 The limited evanescent wave excitation volume makes it possible to m

35 s fit to a model describing diffusion in the evanescent wave excitation.

36 An automated array biosensor based on evanescent-wave excitation has been developed for the de

37 One unknown hampering the interpretation of evanescent-wave excited fluorescence intensities is the

38 Evanescent-wave excited fluorescence technology has been

39 Combining the advantages of evanescent wave fiber optic sensor and microfluidic tech

40 We have developed a disposable evanescent wave fiber optic sensor by coating a molecula

41 An evanescent wave fiber optic sensor for detection of Esch

42 g diode based sensor and the other one is an evanescent wave fiber optic sensor.

43 A "turn-on" evanescent-wave fiber biosensor based on functional nucl

44 The subfield of evanescent wave fluorescence biosensors has also matured

45 We used multicolor evanescent wave fluorescence microscopy imaging to follo

46 We used evanescent wave fluorescence microscopy to observe assem

47 Fluorescence in the film was excited by the evanescent wave from attenuated total reflection spectro

48 e technique uses the unique polarizations of evanescent waves generated by total internal reflection

49 se component of the spin angular momentum of evanescent waves gives rise to lateral optical forces on

50 ver, the effective path length, d(e), of the evanescent wave in an ATR measurement, i.e., the equival

51 This superlens would allow the recovery of evanescent waves in an image via the excitation of surfa

52 rse-spin angular-momentum-density shifts for evanescent waves in magneto-optic waveguide media.

53 r momentum conversion in magneto-optic media evanescent waves in opposite propagation-directions.

54 imit of light, which is causd by the loss of evanescent waves in the far field that carry high spatia

55 sociation kinetics and diffusion through the evanescent wave, in solution, contribute to the fluoresc

56 of contributions from diffusion through the evanescent wave, in solution, has been published previou

57 ctively detected by following changes in the evanescent-wave-induced fluorescence anisotropy of the i

58 lished optical fiber, providing an efficient evanescent wave interaction.

59 t for sensor coating, a waveguide to provide evanescent wave interrogation, and it can be easily exte

60 length objects by transforming the scattered evanescent waves into propagating waves in an anisotropi

61 The metamaterial converts evanescent waves into propagative waves exciting trapped

62 An evanescent wave is generated by total internal reflectio

63 impedance analysis and optical sensing using evanescent waves like SPR.

64 cal spots can actually be formed without any evanescent waves, making far-field, label-free super-res

65 emblies in bacteria lacking MCP complexes by evanescent wave microscopy [6].

66 Using evanescent wave microscopy and green fluorescent protein

67 ugh a single molecular contact is tracked by evanescent wave microscopy as a force is exerted through

68 Here we developed a dual-color evanescent wave microscopy method to simultaneously meas

69 Direct observation of actin filaments by evanescent wave microscopy showed that cofilins from fis

70 Using in vitro evanescent wave microscopy, we demonstrated that GMF pot

71 d neuropeptidergic vesicles by wide-field or evanescent-wave microscopy shows that a separate immobil

72 ssion is due to the enhanced propagating and evanescent wave modes inside the ADNZ medium thanks to t

73 ion spectra obtained in the transmission and evanescent-wave modes are discussed.

74 ch or exceed the distance encompassed by the evanescent wave of the surface plasmon.

75 An evanescent wave optical fiber biosensor based on titania

76 of excitation; that is, it does not require evanescent wave or surface-plasmon excitation.

77 mbdaSH/4 (or lambdapump/8) without involving evanescent waves or subwavelength apertures.

78 ation), the detection volume is a product of evanescent wave penetration depth and distance-dependent

79 ated with the maximum overlap between the IR evanescent wave penetration depth and the analyte diffus

80 ticles synthesized beforehand, or in-situ by evanescent-wave photopolymerization on the fiber.

81 A single evanescent wave possesses a spin component, which is ind

82 ercome the diffraction limit by transforming evanescent waves responsible for imaging subwavelength f

83 compared to previous sizes and geometries of evanescent-wave sensors (e.g., commercially available in

84 Fiber-optic near-ultraviolet evanescent-wave sensors have been constructed, and their

85 strips 30-50 microm thick and 2 mm wide, as evanescent-wave sensors to detect the mid-(IR) evanescen

86 Fiber-optic evanescent wave spectroscopy (FEWS)-FTIR with endoscope-

87 easured by infrared reflection-absorption or evanescent wave spectroscopy) during increase in protein

88 These modes are evanescent waves that form, for example, surface plasmon

89 a conventional biosensor waveguide based on evanescent waves, the ARROW structure is designed to all

90 on, d(p), to estimate the path length of the evanescent wave through the sample.

91 ect on the propagation and penetration of IR evanescent waves through the film.

92 We demonstrate the use of the calibrated evanescent wave to resolve the 20.1 +/- 0.5-nm step incr

93 The measured evanescent wave transfer function was then used to conve

94 ature information of an object is carried by evanescent waves, which exponentially decays in space an