ライフサイエンスコーパス: optical path

1 gnetic fields are accrued gradually along an optical path.

2 lowing absorbance detection in a mere 27 mum optical path.

3 king or super-resolution imaging in a single optical path.

4 pbv/Hz(1/2) to(15)NO using only 45 cm active optical path.

5 he insertion loss and production cost of the optical path.

6 le plane, inside the microscope illumination optical path.

7 ht waves are gradually accumulated along the optical path.

8 able membrane excludes particulates from the optical path.

9 on limit of molecular absorbance in a 27 mum optical path.

10 ver changes occur along the flow cytometer's optical path.

11 king the starlight before it even enters the optical path.

12 using the lens of the tadpole as part of the optical path.

13 index-matching fluid) and positioned in the optical path.

14 nes from atmospheric water vapour within the optical path.

15 d in the center of the reflector to fold the optical path.

16 rp in its orbital angular momentum along the optical path.

17 ht scattered by NPs when passing through the optical path.

18 of changes of the refractive index along an optical path.

19 bsorption attenuates light that travels long optical paths.

20 in amide I band in aqueous solution at large optical paths.

21 monitor distribution of free atoms along the optical path and direct analysis in real time (DART) cou

22 rying frequency applied perpendicular to the optical path and measures the modulation of laser light

23 hyaloid vasculature (important to clear the optical path) and formation of the retinal vasculature (

24 eters where scattering effectively folds the optical path, but instability makes practical realizatio

25 The optical-path can be greatly enhanced and much longer tha

26 a balanced detection module combined with an optical path catered to VCD measurements.

27 d to optimize the linearity and minimize the optical path differences for the dispersed wavenumbers.

28 amples in turbid or opaque liquids since the optical path doesn't pass through the sample.

29 h 1 cm-cuvette, owing to the novel nonlinear optical-path enhancement as well as fast sample switchin

30 GHz), and a time resolution of 200 ps (6 cm optical path in free space).

31 etermined by analyzing the variations in the optical path in the OFS.

32 junction of particle-induced backscatter and optical-path-induced shifts can be used to enhance detec

33 s installed or whenever the flow cytometer's optical path is altered (e.g., lasers, filters or detect

34 either through sample rotation or additional optical paths, is a popular strategy to improve sample c

35 The large optical path length (25 mum), high signal-to-noise ratio

36 od is based on the cell volume dependence of optical path length (OPL) for a light beam passing throu

37 ggests that the dark area has a shorter mean optical path length and about 0.04 per cent by volume mo

38 image quality on optical density by varying optical path length and nanoparticle concentration.

39 ering light within the layer, increasing the optical path length and therefore light absorption by th

40 uted to radically sharp refraction where the optical path length approaches infinity due to the Poynt

41 The channel length and optical path length are therefore tunable.

42 Using a 413 m optical path length astigmatic Herriott cell and two qua

43 in microfluidic channels due to the limited optical path length available in these systems.

44 The noninvasive detection of optical path length changes shows neuronal photoreceptor

45 use of UV-vis bare optical fibers in a long optical path length configuration and the measurement of

46 where two optical fibers are fixed in a long optical path length configuration.

47 attern in the region immediately around zero optical path length difference, while the full HBSI patt

48 e the full HBSI pattern over a wide range of optical path length differences has not yet been well ex

49 e interference patterns over a wide range of optical path length differences.

50 bining three optomechanical parameters in an optical path length equation and a two-degree-of-freedom

51 cattering reduces light absorption along the optical path length from the excitation source to the UV

52 Similar changes in the optical path length have been observed in photoreceptor

53 % lines with a resolution of 4 cm(-1) and an optical path length of 1 mm.

54 The large optical path length of 25 mum allowed for robust spectra

55 A 6V and 10W halogen lamp with an optical path length of 7mm between optical fibers, which

56 ially and temporally resolved changes in the optical path length of the photoreceptor outer segment a

57 hich have the potential to provide increased optical path length over broad bands, and parasitic abso

58 system and a rapid-scanning retro-reflective optical path length scanner.

59 with a temporal resolution of 0.1 ms and an optical path length sensitivity of <4 pm per pixel.

60 ple scattering of light, which increases the optical path length through the sample.

61 a monolithic waveguide as long as 27 m (39 m optical path length), and featuring broadband loss rate

62 is, to a first approximation, independent of optical path length, allowing small-diameter capillaries

63 scopic instrumentation, the variation in the optical path length, resulting from the physical variati

64 ct approach, including issues related to the optical path length, wavelength range, dimensionality of

65 eight (thus, the film thickness) defines the optical path length, which was reduced to between 10 and

66 y of transduced light being dependent on the optical path length.

67 odulator structures with only micrometres of optical path length.

68 he volume of the components and the internal optical path length.

69 sample volume while maintaining the standard optical path length; thin centerpieces with integrated w

70 t controlled-environment measurements of the optical path-length change response of telecommunication

71 of additional information, a new algorithm, optical path-length estimation and correction (OPLEC), i

72 Interference pattern analysis determined the optical path lengths (OPL) associated with reflections f

73 law of superposition, despite the micrometer optical path lengths and the curvatures of the droplets

74 Whereas the long optical path lengths required for light-dispersive compo

75 Here, we demonstrate that longer optical path lengths than afforded by conventional cuvet

76 particularly challenging due to the reduced optical path lengths that are characteristic of microflu

77 fluorescence pattern was caused by increased optical path lengths through the microvilli and microrid

78 ented setup combines high sensitivity, large optical path lengths, and short measurement times and th

79 ge surface-to-volume ratios, and microscopic optical path lengths, both Beer-Lambert's law and the la

80 of proteins in aqueous solution at extended optical path lengths, which allow experiments in flow th

81 sate the reduced light absorption along such optical path, making the impacts of light scattering on

82 For an active optical path of 44 cm and 1-s lock-in time constant mini

83 a transmission diffraction grating into the optical path of a localization-based super-resolution mi

84 uid-crystal based universal polarizer in the optical path of a wide-field light microscope.

85 are generated interferometrically within the optical path of an FPR system.

86 red to a QTA is a consequence of the shorter optical path of the DBD.

87 introduction of a cylindrical lens into the optical path of the Raman excitation laser increases the

88 ough two indistinguishable pairs of disjoint optical paths passing through the masks of interest.

89 been designed for single pass and multi pass optical paths (path length ratio 1:100); it allows simul

90 ions, out-of-plane configurations with short optical paths should be considered.

91 It is the microscope illumination optical path that produces a large cell- and beam-angle

92 cation, such as fiber coupling and increased optical paths, this self-regulated muChopper uses opposi

93 The technique relies on extending the optical path through the sensing volume by suspending di

94 tors, generating resonances by designing the optical path through transverse mode coupling in a casca

95 s to be determined to efficiently tailor the optical path transmitting specific wavelength bands.

96 actively tuning the interference between the optical paths via wavefront shaping, OCIS controls light

97 absorption lines of atmospheric water in the optical path, which was solved by use of wavelengths cen

98 l-fibre array, creating an inherently stable optical path, which we use to demonstrate qubit coherenc

99 , spin and orbital, independently, along the optical path while operating on incident light of any po