ライフサイエンスコーパス: polarizer

1 om following automated gas transfer from the polarizer.

2 qual intensities from both sides of the dual polarizer.

3 polarizer is viewed with a second analyzing polarizer.

4 iode excitation source without an excitation polarizer.

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

6 line in an optical microscope under crossed polarizers.

7 icted that they would replace costly mineral polarizers.

8 bserved with the unaided eye through crossed polarizers.

9 uous imaging of the specimen between crossed polarizers.

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

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

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

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

14 585 nm) light-emitting diode through crossed polarizers and a variable retarder.

15 100 nm thick, without the need for external polarizers and analysers.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

56 Linear polarizers were introduced into both the incident and co

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

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

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

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

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

62 8.2 dB rejection ratios and terahertz linear polarizers with 9.5 dB extinction ratios.

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

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