ライフサイエンスコーパス: Faraday

1 Faraday and Kerr spectroscopies along with spectroscopic

2 Faraday cage designs abound in the literature, often exh

3 Faraday rotation is a fundamental effect in the magneto-

4 Faraday rotation is a magneto-optical effect central to

5 Faraday rotators find applications in optical isolators

6 Faraday to Faraday and Faraday to ion counter time lags

7 Faraday, who studied animal electricity in the Gymnotus

8 7.3 mol g(-1) h(-1), while maintaining > 80% Faraday efficiency for 100 h.

9 A Faraday cup (FC) was used to record the ion flux and tim

10 ials with high dislocation density achieve a Faraday efficiency of 95.4%, an NH(3) yield rate of 20.5

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

12 Our hetero-homogeneous system achieves a Faraday efficiency of ~99% with industrial-level current

13 superior performance in CO(2)RR, achieving a Faraday efficiency of 99 % for CO production (-0.4 V vs.

14 yield of 4.2 mol. g(cat) (-1). h(-1), and a Faraday efficiency of 90 % for ammonia production at -0.

15 nd nanoelectrospray ionization sources and a Faraday plate detector.

16 detectors, such as a mass spectrometer and a Faraday plate.

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

18 This enables its investigation as a Faraday rotator where it displayed a remarkable Verdet c

19 their size and charge and then detected by a Faraday plate detector.

20 eatly exceeds the net charging measured in a Faraday pail/electrometer set up, which brings direct ev

21 4 V vs. RHE) in an H-cell, and maintaining a Faraday efficiency of 98 % at a current density of 270 m

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

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

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

25 en yield of 80.4 mumol/mg protein/day with a Faraday efficiency of 80% at a potential of -0.75 V.

26 rate of 5415+/-26 mmol g(cat) (-1) h(-1) and Faraday efficiency of 99.7+/-0.2 % at -0.3 V vs. RHE, af

27 rate up to 29.2 mug h(-1) mg(-1) (cat.) and Faraday efficiency (FE) up to 27.8 % in nitrogen reducti

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

29 ry they describe between Lorentz's force and Faraday's induction, a principle and a symmetry stunning

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

31 We simulate the Kerr and Faraday effects in realistic experimental setups, and ba

32 gth that probes the magneto-optical Kerr and Faraday effects of Py and YIG, respectively.

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

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

35 In this approach, both of Gauss's laws and Faraday's law are built in as hard constraints, as well

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

37 nction with distinct resonance splitting and Faraday rotation coinciding with the spectral window of

38 Here, we measure magneto-transmission and Faraday rotation in high-mobility encapsulated monolayer

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

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

41 As Faraday rotation alone, however, determines neither the

42 The magneto-optical phenomenon known as Faraday rotation involves the rotation of plane-polarize

43 nfluence magnetic optical phenomena, such as Faraday rotation.

44 omenon of unipolar induction, also known as "Faraday's Paradox".

45 requency domain information for custom-built Faraday cages reveal that maximally conductive cages pro

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

47 hrotron intensity gradient is not limited by Faraday depolarization in the cluster central regions an

48 nic materials, originates from the so-called Faraday B term.

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

50 The CO Faraday efficiency reaches 98% at -0.4 V vs. reversible

51 y using molecular oxygen, achieving combined Faraday efficiencies above 40%.

52 (2)FAPbI(7) using a combination of cryogenic Faraday rotation and transient absorption spectroscopy.

53 y the global sensitivity of current density, Faraday efficiency, and overpotential across 295 electro

54 thods and by working inside a newly designed Faraday cage, and evaluated this from the point of view

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

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

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

58 ectra are consistent with resonance-enhanced Faraday rotation in the region of the Q-band electronic

59 ency demonstrations of nonreciprocity exist, Faraday rotation remains the only known nonreciprocal me

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

61 he impact of chemical structure in thin-film Faraday rotators can be achieved, including the critical

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

63 isation in a way which is indiscernible from Faraday rotation in the interstellar medium for typical

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

65 ne of polarization of light exhibits a giant Faraday rotation of several degrees around the A exciton

66 beats, stimulated spin scattering and giant Faraday rotation.

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

68 The giant Faraday rotation is due to the giant oscillator strength

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

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

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

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

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

74 Impressively, BCN achieves a high Faraday efficiency of 18.9 %, an ammonia yield of 20.9 m

75 nous persistent radio counterpart and a high Faraday rotation measure(6) further distinguish the loca

76 d, 100% magnetic circular dichroism and high Faraday rotation.

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

78 state systems, e.g., via the optical inverse Faraday effect or the phonon inverse Faraday effect.

79 inverse Faraday effect or the phonon inverse Faraday effect.

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

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

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

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

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

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

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

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

88 This suggests that there is Faraday conversion where the radio wave tracks a reversa

89 , which is vital for the prediction of Kerr, Faraday and magneto-circular dichroism spectra of 2D het

90 Owing to the well-known Faraday effect, both the magnon modes are coupled to sin

91 lar assembly of polymers can result in large Faraday effects (Verdet constants = 10(5) degrees T(-1)m

92 These two FRBs have unusually large Faraday rotation measure values(2,3), probably tracing a

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

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

95 -free electrocatalysts still suffer from low Faraday efficiencies and low ammonia yields.

96 edicted relation into the low luminosity-low Faraday rotation measure regime (<1,000 rad m(-2)).

97 n the FRB environment and that FRBs with low Faraday rotation measure may not show a persistent radio

98 iven YBa(2)Cu(3)O(6.48) crystal by measuring Faraday rotation in a magneto-optic material placed in t

99 s could be achieved by adopting the metallic Faraday Cage, which was originally for MR shielding, wit

100 tration in 1883 by Lord Rayleigh and Michael Faraday for the excitation of a single resonant mode by

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

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

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

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

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

106 t because it reduces the contribution of non-Faraday currents.

107 stein condensate, detected by nondestructive Faraday rotation probing, achieves single-shot low-frequ

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

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

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

111 ical arguments predict that, if the observed Faraday rotation measure mostly arises from the persiste

112 e that high transparency and large amount of Faraday rotation in the proximity of resonance frequency

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

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

115 We demonstrate the observation of Faraday's law of induction at the nanoscale and show how

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

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

118 try (MC-ICP-MS) using high-gain 10(13) Omega Faraday cup amplifiers.

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

120 Optical readout based on the magneto-optical Faraday effect was commercialized but soon abandoned bec

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

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

123 t advances in the field of thin-film organic Faraday rotators within the well-established theoretical

124 and high Verdet constants have made organic Faraday rotators a promising alternative to conventional

125 Despite this, organic Faraday rotators have not been developed to address near

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

127 The catalyst shows an outstanding Faraday efficiency (~30 %) and high yield (~113 mug h(-1

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

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

130 mmetry breaking, however, generally requires Faraday rotators or nanofabricated polarization-preservi

131 t room-temperature, picosecond time-resolved Faraday ellipticity/rotation (TRFE/R) measurements of th

132 Through time-resolved Faraday rotation and Kerr ellipticity, we found that the

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

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

135 Femtosecond time-resolved Faraday rotation spectroscopy reveals the instantaneous

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

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

138 panning 17 months, which show that the FRB's Faraday rotation is highly variable and twice changes si

139 Cavity attenuated phase shift Faraday rotation spectroscopy has been developed and dem

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

141 ought fundamental question in science, since Faraday's 1857 work.

142 This strong Faraday rotation, which is amongst the highest value kno

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

144 Typically, B term Faraday responses are weak.

145 We also verify that Faraday-based phase-conjugate mirrors hold the genuine p

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

147 The Faraday effect is a representative magneto-optical pheno

148 The Faraday instability appears on liquid baths submitted to

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

150 yrin and phthalocyanine derivatives, and the Faraday A-term describes the electronic origin of the ma

151 ent manners, via temporal modulation and the Faraday effect, to synthesize tunable non-Abelian gauge

152 of the strong magnetic field imposed by the Faraday effect.

153 provide an alternative means to enhance the Faraday rotation of low symmetry systems and clarify the

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

155 ime modulation of the medium involved in the Faraday instability can act as a phase-conjugate mirror-

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

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

158 f arbitrary shapes to spatially localize the Faraday instability.

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

160 A brief history of the Faraday cage and a simplified theoretical approach intro

161 ore than 175 years, our understanding of the Faraday effect in solid-state organic materials remains

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

163 experimental evidence of the ability of the Faraday instability to generate counterpropagating phase

164 s show irregular short-time variation of the Faraday rotation measure (RM), which scrutinizes the den

165 At lower values of the Faraday rotation measure, the expected radio luminosity

166 pin resonance and a long-lived offset of the Faraday signal are hallmarks of coherent spin switching

167 evaluate candidate chromophores based on the Faraday A, B, and C term framework presented herein.

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

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

170 nents such as optical isolators based on the Faraday rotation, hindering the miniaturization and inte

171 The CoMoO(4) electrocatalyst possessed the Faraday efficiencies (FEs) of CO and CH(4) up to 56.80%

172 ghting the physical principles producing the Faraday effect.

173 etic circular dichroism spectroscopists: the Faraday A, B, and C terms.

174 The fact that the Faraday cage composition most often goes unreported unde

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

176 Unlike the Faraday effect, the optical activity provokes rotation o

177 allow for concentration calculation via the Faraday Law: The sample volume must be precisely defined

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

179 defect, curves the geometry such that these Faraday lines are channeled preferentially by the arrays

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

181 x 10(5) deg T(-1)m(-1) at 700 nm assigned to Faraday A-term activity.

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

183 Specifically, the disclination leads to Faraday lines of effective magnetic flux that run from t

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

185 The ubiquitous Faraday cage, an experimental component particularly ess

186 denced by a strong ( ~ 1 degrees ) ultrafast Faraday rotation ( ~ 20 ps).

187 egrating the current-time response and using Faraday's Law.

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

189 dels and demonstrate it experimentally using Faraday wave instabilities.

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

191 han purely electrochemical predictions using Faraday's law.

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

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

194 modifiable for magnetic field detection via Faraday rotation.

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

196 o Nano-Amp) amplification system paired with Faraday cup detectors has a large dynamic range and low