ライフサイエンスコーパス: polarizer

1 axis, which corresponds to the direction of polarizer.

2 om following automated gas transfer from the polarizer.

3 qual intensities from both sides of the dual polarizer.

4 polarizer is viewed with a second analyzing polarizer.

5 iode excitation source without an excitation polarizer.

6 ich are indirectly validated with a rotating polarizer.

7 n current aligns with the Neel vector of the polarizer.

8 ra-Red (IR) transmission imaging under cross polarizers.

9 frequency selective surfaces, modulators and polarizers.

10 dard optical elements such as waveplates and polarizers.

11 on of a bright optical flash between crossed polarizers.

12 is the basis for the operation of wire grid polarizers.

13 line in an optical microscope under crossed polarizers.

14 icted that they would replace costly mineral polarizers.

15 bserved with the unaided eye through crossed polarizers.

16 uous imaging of the specimen between crossed polarizers.

17 , such as polarization rotators and circular polarizers.

18 d in the delivered gas, starting with an "in-polarizer" (129)Xe polarization of 19%.

19 ntensities of axonemes viewed with different polarizer-analyzer settings differ from those calculated

20 als oriented in various directions, with the polarizer and analyzer arranged in different configurati

21 This allows the use of fixed polarizer and analyzer in a crossed configuration and co

22 on hemisphere-based SI lens, metal-wire-grid polarizer and analyzer, a continuous-wave 0.6 THz ([Form

23 magnet (F2) spin valve, where F1 acts as the polarizer and F2 the analyser.

24 585 nm) light-emitting diode through crossed polarizers and a variable retarder.

25 100 nm thick, without the need for external polarizers and analysers.

26 decays were acquired with toggling or static polarizers and fitted according to the standard protocol

27 rcially available optical components such as polarizers and mirrors, and therefore, provides a signif

28 ssibilities for efficient ultrathin circular polarizers and narrow-band thermal emitters of circularl

29 m splitters, terahertz wave plates, circular polarizers and other polarization devices.

30 ch as dynamically tunable terahertz circular polarizers and polarization modulators for terahertz rad

31 at depend on the relative orientation of the polarizers and the membrane normal, thus demonstrating t

32 g several external optical elements, such as polarizers and wave plates, along with conventional phot

33 that produced the first large-aperture light polarizers and, in turn, the Polaroid empire.

34 simple filtration in the cryostat of the DNP polarizer, and a pure hyperpolarized solution is collect

35 e sample is located between rotating crossed polarizers, and camera images are obtained at each point

36 opic displays, polarization encoding, chiral polarizers, and colorimetric chiral biosensing.

37 can also realize tunable metalenses, active polarizers, and flat spatial light modulators.

38 and complicated optical systems with lenses, polarizers, and mechanical spools, which are complex and

39 que, diffraction gratings, bilayer wire-grid polarizers, and resonant metal mesh long-pass filters ar

40 Optical polarizers are a typical class of such materials, but an

41 In this method, two polarizers are combined into the conventional THz-TDS sy

42 arimeter is constructed by packaging a micro-polarizer array on top of an InGaAs sensor.

43 duce here a compact helium-free 1-T tabletop polarizer as a simple and low-cost alternative.

44 tically transparent graphene-based wire-grid polarizer at microwave frequencies (X band).

45 nstrate a highly efficient pure spin current polarizer at room temperature using a single-domain anti

46 s such as lenses, phase plates, wave plates, polarizers, beamsplitters, as well as polarization-switc

47 erature which involves toggling the emission polarizer before fitting linear combinations of the I(VV

48 the I(VV)(t) and I(VH)(t) decays with static polarizers before fitting them globally.

49 spectrum filter (resonant transmission) to a polarizer (broadband transmission) for TM polarized ligh

50 A pure spin current polarizer, capable of controlling both its transmittance

51 birefringence when observed between crossed polarizers, characteristic of amyloid structures.

52 -yield spin-exchange optical pumping (129)Xe polarizer, custom-built radiofrequency coils, and an opt

53 the LC as a function of the orientation of a polarizer; data analysis condenses the information prese

54 However, this global polarizer does not appear to act as a localized, spatial

55 Optical polarizers encompass a class of anisotropic materials th

56 Such materials play an important role as polarizers, filters, and waveplates in photonic devices

57 " large-scale ( approximately 1 L/h) (129)Xe polarizer for clinical, preclinical, and materials NMR a

58 nsmission amplitudes interfere at the output polarizer; for special polarization angles, which depend

59 anning calorimetry, and show, using a simple polarizer-free electro-optic cell, that the reflected co

60 ws and tags, new material properties such as polarizer-free operation and tunable memory of a written

61 d phenomena is demonstrated by nanocomposite polarizers from molybdenum sulfide (MoS(2)), MXene and g

62 near grating (SABLG), serving as a wire grid polarizer in the mid-wavelength infrared (MWIR) region.

63 y employing a liquid-crystal based universal polarizer in the optical path of a wide-field light micr

64 evices, and in narrowband filters and linear polarizers in reflection mode.

65 We use the approach to create ideal polarizers in the terahertz frequency range and, by comb

66 gned, limiting their use to stationary cross-polarizers in, for example, liquid crystal displays.

67 Such a simple benchtop polarizer, in combination with hyperpolarizing solid mat

68 at various orientations with respect to the polarizers, including filament orientations perpendicula

69 rises 1.6 wt.% of bulk sediment, and crossed polarizers indicate that the meltglass is isotropic.

70 Thus, the leukocyte polarizer is a dual-role phosphoinositide-transfer prote

71 ded to the excitation path and a Glan-Taylor polarizer is added to the collection path, and these mod

72 xperiment in addition to a conventional dDNP polarizer is simple and readily assembled.

73 The emission passing through the dual polarizer is viewed with a second analyzing polarizer.

74 light propagating through the modulator and polarizers is intensity modulated with a wide acceptance

75 ion of transmitted through a pair of crossed polarizers light, is achieved with 4.5 V/mum with a sub-

76 The modulator is placed between optical polarizers; light propagating through the modulator and

77 The rotating-polarizer method was used to separate the optical effect

78 polarization dependence, need for additional polarizers, narrow operation bandwidth, being limited wi

79 ultiplier tube and eliminates the need for a polarizer on the emission path.

80 s were transferred from a low magnetic field polarizer operating at 1.76 mT to a 4.7 T animal MR scan

81 between parallel polars instead of either a polarizer or analyzer alone, the fluorescence polarizati

82 in polarization, and hence be used as a spin polarizer or detector.

83 n wavelengths, orientation of the excitation polarizer, or fluorophore concentration in the reference

84 frozen, solid sample from the low-T, high-B polarizer, passing it through low field (B < 100 G) to f

85 Linear gratings polarizers provide remarkable potential to customize the

86 Microscope examination under cross polarizers provided confirmation of ordered crystals.

87 ference fringe image on the interface with a polarizer-quartz wedge depolarizer combination.

88 be laser is similarly split (with an optical polarizer) replicating the detection chain to obtain two

89 d by adjusting the surrounding medium or the polarizer setting.

90 constitutes an ultrathin, broadband circular polarizer that may be directly integrated within nanopho

91 urements and simultaneously act as wire-grid polarizers that protect the underlying substrate from di

92 k this process, we compared a prototype PHIP polarizer to a state-of-the-art dissolution dynamic nucl

93 hat act synergistically as a dual macrophage polarizer to promote the M1 phenotype and suppress the M

94 at the Earth's magnetic field) from the PHIP polarizer to the 47.5 mT low-field MRI.

95 hyperpolarized sample travels from the dDNP polarizer to the NMR spectrometer, it goes through a fie

96 ew optical components such as liquid crystal polarizers to a typical Raman setup.

97 y adjusts the incident light using a pair of polarizers to precompensate the IR absorption by water w

98 ri-image splitter outfitted with appropriate polarizers, to concurrently excite and collect fluoresce

99 By introducing a tilted THz ultra-broadband polarizer, we split the THz beam in two orthogonal polar

100 Using partial polarizers, we perform a filtering process to maximize t

101 Linear polarizers were introduced into both the incident and co

102 s and show uniform textures between circular polarizers when suspended in sub-millimeter size grids a

103 present results detailing a low-field SABRE polarizer which provides well-controlled experimental co

104 We anticipate that this pure spin current polarizer will serve as a building block for spintronics

105 zation can be detected visually using a dual polarizer with adjacent sections oriented orthogonally t

106 lly controlled, automated parahydrogen-based polarizer with in situ detection capability.

107 anical light modulation by rotating a linear polarizer with respect to a quarter wave plate continuou

108 8.2 dB rejection ratios and terahertz linear polarizers with 9.5 dB extinction ratios.

109 oelectronic applications including terahertz polarizers with nearly perfect extinction ratios and bro

110 by embedding an imprinted bilayer wire-grid polarizer within the CQDs.

111 on to a (13) C nucleus using a para-hydrogen polarizer yielded a polarization of 0.013%.