ライフサイエンスコーパス: polarimetry

1 udies in fluid dynamics, remote sensing, and polarimetry.

2 delivery and the 5 mm NMR tube employed for polarimetry.

3 ), which can be detected by optical harmonic polarimetry.

4 ds with high-precision time-domain terahertz polarimetry.

5 rified MBCHs then were determined by digital polarimetry.

6 al set-up for joint parameter estimation for polarimetry.

7 ted fibers were analyzed with Mueller matrix polarimetry.

8 ture, as judged by both NMR spectroscopy and polarimetry.

9 rovement in detecting earliest glaucoma with polarimetry.

10 the assessment of the RNFL by scanning laser polarimetry.

11 age-related macular degeneration (AMD) using polarimetry.

12 dates for high-performing direct full-stokes polarimetry.

13 r was quantified using in situ low-field NMR polarimetry and additionally verified using a 0.35 T cli

14 Low chiral signatures were measured by polarimetry and electronic circular dichroism, whereas m

15 approach exhibits high-accuracy full-Stokes polarimetry and high-resolution real-time polarization i

16 i through optical second harmonic generation polarimetry and in situ TEM electrical testing on single

17 ng scanning laser tomography, scanning laser polarimetry and optical coherence tomography offer more

18 nd could find applications in hyper-spectral polarimetry and scanning microscopy.

19 vanced experimental technique called Mueller polarimetry and state-of-the-art numerical simulations.

20 The method is based on double Stokes-Mueller polarimetry and uses linear and circular incident and ou

21 l coherence tomography (OCT), scanning laser polarimetry, and confocal scanning laser ophthalmoscopy.

22 erve fiber layer observation, scanning laser polarimetry, and confocal scanning laser tomography may

23 demonstrate high-multipole nonlinear optical polarimetry as a sensitive and mode selective probe of S

24 Here, we introduce two-dimensional polarimetry as means of direct imaging of the valley pse

25 icient of variation 2%-2.9%), scanning laser polarimetry (coefficient of variation 2.6%-4.5%), and co

26 optical coherence tomography, scanning laser polarimetry, confocal scanning laser ophthalmoscopy, pup

27 orrelation between CPA measured with corneal polarimetry (CPA by P(IV) [fourth Purkinje image]) and S

28 iagnostic Technologies, Inc., San Diego, CA) polarimetry data and to evaluate the techniques' ability

29 tion angles are directly calculated from the polarimetry data obtained in a single scan, while other

30 pattern was analyzed by Fourier analysis of polarimetry data.

31 ng are presented for a new spherical neutron polarimetry device utilizing high-T(c) superconducting Y

32 inear polarimetry method named double Stokes polarimetry (DSP) for quick characterization of chiral C

33 chiroptical properties were determined from polarimetry, electronic (ECD), and vibrational (VCD) cir

34 erties of compounds 2-4 were determined from polarimetry, electronic circular dichroism (ECD), and vi

35 d 1RXS J170849.0-400910 by the Imaging X-ray Polarimetry Explorer (IXPE) opened up a new avenue to st

36 magnetar 4U 0142+61 using the Imaging X-ray Polarimetry Explorer and found a linear polarization deg

37 f the XRB Cygnus X-1 using the Imaging X-ray Polarimetry Explorer.

38 the Galactic Centre using the Imaging X-ray Polarimetry Explorer.

39 w variant of continuous-wave cavity-enhanced polarimetry for detecting the optical activity of two en

40 one of its two modes of operation: optimized polarimetry for Jones matrix measurements.

41 , we demonstrate the potential of wide-field polarimetry for rapid inspection of opto-valleytronic de

42 batic transitions to adapt spherical neutron polarimetry for use with pulsed neutron sources, thereby

43 measured by three techniques: scanning laser polarimetry (GDx ECC; Carl Zeiss Meditec, Dublin, CA), c

44 ds regression analysis (MRA), scanning laser polarimetry (GDx enhanced corneal compensation; Glaucoma

45 birefringence was measured by scanning laser polarimetry (GDx VCC; Carl Zeiss Meditec, Inc., Dublin,

46 g Laser Ophthalmoscopy (HRT), Scanning Laser Polarimetry (GDx) and Optical Coherence Tomography (OCT)

47 ng, Heidelberg, Germany), and scanning laser polarimetry (GDx-VCC; Carl Zeiss Meditec, Inc., Dublin,

48 Imaging Mueller polarimetry has already proved its potential for biomedi

49 Scanning laser polarimetry, Heidelberg retinal tomography and optical c

50 erature concerning the use of scanning laser polarimetry, Heidelberg retinal tomography and optical c

51 supports the assumption that imaging Mueller polarimetry holds promise for the fast and accurate coll

52 gment birefringence can be determined from a polarimetry image of the Henle fiber layer.

53 ngence of normal eyes were determined from a polarimetry image of the Henle fiber layer.

54 Each polarimetry image was compared with the corresponding au

55 otographs, were quantified in three types of polarimetry images: (1) a depolarized light image result

56 With this polarimetry imaging method, subretinal tissues such as t

57 FL retardance was measured by scanning laser polarimetry in 10-minute intervals for 30 minutes while

58 Using two-photon fluorescence polarimetry in giant unilamellar vesicles and in the pla

59 Here we report imaging circular polarimetry in the near-infrared and Monte Carlo modelli

60 In contrast to polarimetry, in which the polarization state of the exit

61 Polarimetry is a noninvasive method that uses polarised

62 Spherical neutron polarimetry is a powerful polarized neutron scattering t

63 Developing direct full-stokes imaging polarimetry is essential for various applications but re

64 ization phenomenon was investigated by laser polarimetry, mass-tagged pseudo-enantiomers in conjuncti

65 The SHG polarimetry measurements identify symmetries in differen

66 uced in a laboratory--over 340 megagauss--by polarimetry measurements of self-generated laser harmoni

67 piezoresponse and second harmonic generation polarimetry measurements, our workflow reveals behaviour

68 times greater than those observed in optical polarimetry measurements, thus allowing picogram quantit

69 e their topological nature through far-field polarimetry measurements.

70 Here, we develop an optically-controlled polarimetry memtransistor based on a van der Waals heter

71 We present a reduced nonlinear polarimetry method named double Stokes polarimetry (DSP)

72 We performed optical polarimetry observations of a TDE, AT 2020mot.

73 tility of the device is demonstrated for NMR polarimetry of hyperpolarized (129)Xe gas and [1-(13)C]p

74 signed for the purpose of ultralow-field NMR polarimetry of hyperpolarized contrast media.

75 The polarimetry of the resulting coherent oscillation amplit

76 Here we report high-resolution imaging and polarimetry of those light echoes, which allow us to set

77 stimuli-responsive polymers, Mueller matrix polarimetry offers an important advantage requiring a fe

78 we employ resonant soft x-ray scattering and polarimetry on thin films of bilayer La(3)Ni(2)O(7) to d

79 Two-dimensional NMR spectroscopy and polarimetry provided a deeper understanding of the under

80 X-ray polarimetry provides a unique diagnostic to study the lo

81 e RNFL in certain conditions, it lacks laser polarimetry's ability to detect microtubule changes.

82 articularly, the anti-glare recognition with polarimetry saves an order of magnitude energy compared

83 opy, X-ray diffraction analysis, and optical polarimetry show that the spherulites are composed of he

84 L measurements acquired using scanning laser polarimetry (SLP) and optical coherence tomography (OCT)

85 ning laser tomography (CSLT), scanning laser polarimetry (SLP) and photographic imaging of the optic

86 s RNFL retardance measured by scanning laser polarimetry (SLP) and T is RNFL thickness measured by op

87 It was hypothesized that scanning laser polarimetry (SLP) compared with OCT might reveal the sta

88 is assumed, the conversion of scanning laser polarimetry (SLP) phase-retardation measurements to RNFL

89 Scanning laser polarimetry (SLP) results can be affected by an atypical

90 Scanning laser polarimetry (SLP) reveals abnormal retardance of birefri

91 ies for glaucoma detection of scanning laser polarimetry (SLP) with enhanced corneal compensation (GD

92 l coherence tomography (OCT), scanning laser polarimetry (SLP), and visual evoked potentials.

93 amine the association between scanning laser polarimetry (SLP), using enhanced (ECC) and variable cor

94 oherence tomography (OCT) and scanning laser polarimetry (SLP).

95 sing and streak imaging with stereoscopy and polarimetry, SP-CUP enables video-recording of five phot

96 ixed compensation, as used in the commercial polarimetry system.

97 Here we use X-ray polarimetry to determine the resistivity of a sulphur-do

98 optical depolarization rate, allowing tissue polarimetry to guide DESI-MS analysis for rapid MS profi

99 Here we use time-resolved polarimetry to reveal critical nematic fluctuations in u

100 neural network(15,16) to achieve full-Stokes polarimetry together with wavelength detection simultane

101 trast media (which was compared to the (13)C polarimetry using a more established technology of bench

102 Using time-resolved optical polarimetry, we further show that the enhanced mechanica

103 Using Mott polarimetry, we probed the spin degrees of freedom and d

104 Proton NMR spectroscopy and polarimetry were used to measure the rates of deuterium

105 iral analysis, as enabled by cavity-enhanced polarimetry, which allows for accurate unambiguous enant

106 rate a spectroscopic phenomenon, superchiral polarimetry, which can rapidly characterize ligand-induc

107 in report a self-powered, direct full-Stokes polarimetry with a high detectivity up to 1.2 x 10(12) J

108 c disc stereophotographs, and scanning laser polarimetry with enhanced corneal compensation.

109 S, which is based on division-of-focal-plane polarimetry with four parallel linear polarization chann

110 ase their application in full-stokes imaging polarimetry with the lowest detection errors yet.

111 ol participant also underwent scanning laser polarimetry with variable corneal compensation (GDx VCC)

112 The scanning laser polarimetry with variable corneal compensation (GDx VCC)

113 In scanning laser polarimetry with variable corneal compensation (SLP-VCC)