ライフサイエンスコーパス: Faraday

1 Faraday and Kerr spectroscopies along with spectroscopic

2 Faraday to Faraday and Faraday to ion counter time lags

3 Faraday, who studied animal electricity in the Gymnotus

4 ion amount of those oxides and can achieve a Faraday efficiency of about 98% for H2O2 production.Prod

5 nd nanoelectrospray ionization sources and a Faraday plate detector.

6 metallic enclosure will effectively act as a Faraday cage to electromagnetic radiation and therefore

7 Among the superionic conductors that show a Faraday transition - the continuous increase in the ioni

8 The detection (using a Faraday cup) of charges transferred to the cup by the io

9 d ion current in IFT-IMS experiments using a Faraday plate.

10 Faraday to Faraday and Faraday to ion counter time lags were determined and cor

11 In thicker films, the Kerr and Faraday angles can be enhanced by choice of film thickne

12 opological theta-term to obtain the Kerr and Faraday rotations in a variety of geometries.

13 ms thinner than the wavelength, the Kerr and Faraday rotations, determined by the separation between

14 both having electron-impact ion sources and Faraday cup collector systems.

15 abilities, such as Benjamin-Feir, Turing and Faraday instability, which play a critical role in the s

16 In more recent times da Vinci and Faraday provide role models for scrupulous recording of

17 As Faraday rotation alone, however, determines neither the

18 g to the "disruptive discharge" described by Faraday.

19 A 512-channel Faraday-strip array detector has been developed and fitt

20 the Benjamin-Feir and the purely dispersive Faraday instability.

21 rium iron garnet (Ce:YIG) thin films display Faraday and Kerr rotation (rotation of light polarisatio

22 e experimentally demonstrate the dissipative Faraday instability induced by spatially periodic zig-za

23 mation optics has been developed, exploiting Faraday's picture of electric and magnetic fields as lin

24 the specimen, rotation produced by the first Faraday rotator is cancelled by the second.

25 A second-generation Faraday-strip array detector has been coupled to an indu

26 beats, stimulated spin scattering and giant Faraday rotation.

27 stor based on a linear optical effect: giant Faraday rotation induced by a single electronic spin in

28 The FPC consists of an array of gold Faraday cups, each coupled to its own integrator, with i

29 The FPC employs an array of gold Faraday cups, each with its own charge-integrating circu

30 fore, it is possible to detect gravitational Faraday rotation by monitoring the X-ray polarization of

31 The effect of gravitational Faraday rotation was predicted in the 1950s, but there i

32 By creating a novel aperture grid/Faraday plate design, a high-pressure IMS (HPIMS) system

33 nd identify the optimal bias ranges for high Faraday efficiencies.

34 uced magnetic field arising from the inverse Faraday effect (IFE).

35 components that we attribute to the inverse Faraday effect and optical spin-transfer torque, respect

36 el does not preclude the role of the inverse Faraday effect but removes the necessity that the opto-m

37 The inverse Faraday effect is approximately the same in Fe, Ni and C

38 ar momentum induced optically by the inverse Faraday effect will provide switching with one single fe

39 field within the media, known as the inverse Faraday effect.

40 The samples showed the highest IR Faraday rotation reported for thin films of Ce:YIG, whic

41 Here we present a mid-IR Faraday rotation spectrometer (FRS) for detection of NO

42 all thickness, electrode spacing and length, Faraday shield thickness, excitation wave forms, and amp

43 On the basis of a low Faraday rotation (12.0 +/- 0.7 radians per square meter)

44 was influenced by his contemporary, Michael Faraday at the Royal Institution, and by two colleagues

45 cal discoveries of his contemporary, Michael Faraday, and thought of the brain as having battery like

46 Faradaurate-279 (F-279) in honor of Michael Faraday's (1857) pioneering work on nanoparticles.

47 ction of Fe isotope ion beams using multiple Faraday collectors facilitates high-precision isotope ra

48 near polarization was detected, and hence no Faraday rotation measure could be determined.

49 The normal Faraday plate collector electrode was replaced with an e

50 antages are demonstrated by means of a novel Faraday-strip array detector coupled to a Mattauch-Herzo

51 coulometric stripping, determinations obeyed Faraday's law over a reasonably wide range of operating

52 The possible detection of Faraday rotation of linearly polarized photons emitted b

53 mode conversion, the waveguide equivalent of Faraday Rotation (FR).

54 s today dominantly rely on the phenomenon of Faraday rotation in magneto-optic materials.

55 re that mimics the nonreciprocal property of Faraday rotation without using any magnetic or electric

56 By placing one Faraday rotator before and one after the specimen, rotat

57 We use optical Faraday rotation (OFR) to probe nuclear spins in real ti

58 surface with Fermi arcs, there is no Kerr or Faraday rotation but the electric field develops a longi

59 the interference was detected with all other Faraday cups except the center cup.

60 A transportable prototype Faraday rotation spectroscopic system based on a tunable

61 s higher than 5 tesla, we observed quantized Faraday and Kerr rotations, whereas the dc transport is

62 Time-resolved Faraday rotation experiments were performed in which the

63 tals has been investigated via time-resolved Faraday rotation measurements.

64 Femtosecond time-resolved Faraday rotation spectroscopy reveals the instantaneous

65 We use off-resonant Faraday rotation to passively detect the magnetization n

66 t the examination of archival data revealing Faraday rotation in the fast radio burst FRB 110523.

67 Since Faraday's pioneering work on gold colloids, tremendous s

68 In this study, Faraday rotation was significantly enhanced through the

69 The Faraday detector of a drift tube for an ion mobility spe

70 The Faraday effect is a representative magneto-optical pheno

71 The Faraday rotation of ZnO/Ag(NPs)/Fe was enhanced 58 fold

72 rameter, z the formal peptide valence, F the Faraday constant, and phi the membrane surface potential

73 wire and measuring the modifications in the Faraday voltage as the stress is varied.

74 ible hydrogen electrode (RHE)), increase the Faraday efficiency (>90%), markedly improve stability (c

75 We have measured the Faraday rotation toward a large sample of polarized radi

76 alizes a gate-tunable magnonic analog of the Faraday effect, and demonstrate its application in THz s

77 ties in conventional approaches based on the Faraday effect, alternative solutions have resorted to n

78 Here we report on the Faraday rotation induced in the prominent 3D topological

79 nondestructive spin measurement, through the Faraday effect, and coherent spin manipulation, through

80 The sensitivity of these Faraday plate ion detectors are limited by thermal (John

81 ear dynamic range remain impressive for this Faraday-based detector system, limits of detection and i

82 Faraday to Faraday and Faraday to ion counter time lags were determ

83 type instrument has been developed using two Faraday rotators under computer control to change the an

84 Charge density was determined using Faraday's law and the significance of electron transfer

85 e silicon-on-insulator (SOI) isolators using Faraday Rotation are here realized to fill the 'missing

86 han purely electrochemical predictions using Faraday's law.

87 nown analytes from the EC-array signal using Faraday's law can eliminate the need for isotopically la

88 ors, and ion mobility spectrometers, utilize Faraday plate designs in which ionic charge is collected

89 modifiable for magnetic field detection via Faraday rotation.

90 intensity counting statistics combined with Faraday cup detection noise limit the precision on the d