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1 f and 6d electronic states by means of X-ray magnetic circular dichroism.
2 ucting quantum interference device and X-ray magnetic circular dichroism.
3 n behavior and geometry in solution by using magnetic circular dichroism.
4 opic methods, including X-ray absorption and magnetic circular dichroism.
5 orbital moment of Co, as observed with x-ray magnetic circular dichroism.
6 netometry, ferromagnetic resonance and X-ray magnetic circular dichroism.
7 sion electron microscopy combined with x-ray magnetic circular dichroism.
8 defined by electrodic reduction monitored by magnetic circular dichroism.
9 ersal-symmetry-breaking sensitivity of X-ray magnetic circular dichroism(12) with magnetic linear dic
10 imagnetic material, the AOS is attributed to magnetic circular dichroism and angular momentum transfe
14 e trivalent Sm dopant, as confirmed by X-ray magnetic circular dichroism and first-principles calcula
15 insights into these topics, revealing strong magnetic circular dichroism and giant Kerr signals in at
16 light near to the 50% maximum allowed, 100% magnetic circular dichroism and high Faraday rotation.
17 ed by different probing depths, namely X-ray magnetic circular dichroism and photoelectron spectrosco
19 udy, we have examined these two enzymes with magnetic circular dichroism and UV-visible absorption sp
20 element-specific techniques, including X-ray magnetic circular dichroism and X-ray absorption spectro
21 /Pd trilayer system is investigated by x-ray magnetic circular dichroism and x-ray resonant magnetic
23 element-specific measurement technique x-ray magnetic circular dichroism, and determined the full mag
25 nge, we have employed electronic absorption, magnetic circular dichroism, and electron paramagnetic r
26 copic techniques, including resonance Raman, magnetic circular dichroism, and electron paramagnetic r
27 f wild-type nNOS with UV-visible absorption, magnetic circular dichroism, and electron paramagnetic r
28 cterization (absorption, circular dichroism, magnetic circular dichroism, and electron paramagnetic r
29 tiometry and characterization by UV-visible, magnetic circular dichroism, and electron paramagnetic r
30 been characterized by electronic absorption, magnetic circular dichroism, and electron paramagnetic r
31 yme variants by using electronic absorption, magnetic circular dichroism, and electron paramagnetic r
33 (2+)Cbi (+) by using electronic absorption, magnetic circular dichroism, and electron paramagnetic r
34 the CFeSP, we have combined resonance Raman, magnetic circular dichroism, and EPR spectroscopic metho
35 bauer, resonance Raman, variable-temperature magnetic circular dichroism, and EPR spectroscopies.
36 e using element specific time-resolved x-ray magnetic circular dichroism, and ferromagnetic resonance
38 UV-visible absorption, variable temperature magnetic circular dichroism, and resonance Raman data, i
41 d using x-ray absorption spectroscopy, x-ray magnetic circular dichroism, and resonant inelastic x-ra
42 device magnetometry, surface-sensitive X-ray magnetic circular dichroism, and spatially resolved magn
44 s probed by UV-visible, variable temperature magnetic circular dichroism, and x-ray absorption spectr
45 ronic spectra of porphycenes: Absorption and magnetic circular dichroism are discussed, together with
46 oment, which was directly confirmed by X-ray magnetic circular dichroism, as an element-specific prob
50 produces a six-coordinate circular dichroism/magnetic circular dichroism (CD/MCD) spectra for ferrous
52 cterized by electron paramagnetic resonance, magnetic circular dichroism, circular dichroism, and ele
53 d resonant X-ray absorption spectroscopy and magnetic circular dichroism, combined with hard X-ray ph
57 sion microscopy using element-specific X-ray magnetic circular dichroism effects as magnetic contrast
58 examined the absorption, circular dichroism, magnetic circular dichroism, electron paramagnetic reson
59 of low-temperature electronic absorption and magnetic circular dichroism, electron paramagnetic reson
60 circular dichroism, and variable-temperature magnetic circular dichroism, electron paramagnetic reson
61 Electron Microscope (TEM) to obtain Electron Magnetic Circular Dichroism (EMCD) signals as a function
62 -visible absorption and variable-temperature magnetic circular dichroism, EPR, resonance Raman and Mo
63 (4) film exhibit an enhanced, almost-perfect magnetic circular dichroism for a narrow photon energy w
64 ructure of altermagnetic RuO(2) by detecting magnetic circular dichroism in angle-resolved photoemiss
66 nd atomic site specific Fe L(2,3)-edge X-ray magnetic circular dichroism indicated that MtoA directly
67 etization, indicating that the present X-ray magnetic circular dichroism is not arising from the conv
71 using electronic absorption, low-temperature magnetic circular dichroism (MCD) and variable-temperatu
82 itored by atomic absorption spectrometry and magnetic circular dichroism (MCD) shows that the enzyme
86 Ferrous M79A and H229A HtsA mutants possess magnetic circular dichroism (MCD) spectra that are simil
88 consistent with circular dichroism (CD) and magnetic circular dichroism (MCD) spectroscopic data and
89 ave employed electronic absorption (Abs) and magnetic circular dichroism (MCD) spectroscopic techniqu
90 variable-temperature, variable-field (VTVH) magnetic circular dichroism (MCD) spectroscopies (FeII s
92 aramagnetic resonance (EPR), absorption, and magnetic circular dichroism (MCD) spectroscopies show th
99 n-deficient bulk SrTiO3-delta crystals using magnetic circular dichroism (MCD) spectroscopy and SQUID
100 s heme identity for LPO, we used comparative magnetic circular dichroism (MCD) spectroscopy of LPO ve
102 ectronic absorption and variable-temperature magnetic circular dichroism (MCD) spectroscopy to experi
103 is described with an emphasis on the use of magnetic circular dichroism (MCD) spectroscopy to valida
104 ngle X-ray scattering (GIWAXS) spectroscopy, magnetic circular dichroism (MCD) spectroscopy, and time
105 ed photodissociation (IRPD), absorption, and magnetic circular dichroism (MCD) spectroscopy, coupled
110 e spin-sensitive responses to CP light using magnetic circular dichroism (MCD) that could allow up to
111 Q) electron paramagnetic resonance (EPR) and magnetic circular dichroism (MCD) yields two intermediat
112 y absorption fine structure (XAS/EXAFS), and magnetic circular dichroism (MCD)) with ab initio theore
114 uency electron paramagnetic resonance (EPR), magnetic circular dichroism (MCD), and nuclear magnetic
115 In the current study, resonance Raman (rR), magnetic circular dichroism (MCD), and nuclear magnetic
116 on, we employed electronic absorption (Abs), magnetic circular dichroism (MCD), and resonance Raman s
117 K-edge X-ray absorption, UV-vis absorption, magnetic circular dichroism (MCD), and resonance Raman s
118 X were studied with circular dichroism (CD), magnetic circular dichroism (MCD), and variable temperat
120 ng a combination of circular dichroism (CD), magnetic circular dichroism (MCD), and variable-temperat
123 In this study, circular dichroism (CD), magnetic circular dichroism (MCD), and variable-temperat
124 A combination of circular dichroism (CD), magnetic circular dichroism (MCD), and variable-temperat
125 als were studied by magnetic susceptibility, magnetic circular dichroism (MCD), and X-ray magnetic ci
126 riety of spectroscopic methods ((119)Sn-NMR, magnetic circular dichroism (MCD), electron paramagnetic
127 UV/visible absorption, variable-temperature magnetic circular dichroism (MCD), EPR, and resonance Ra
128 bination of near-IR circular dichroism (CD), magnetic circular dichroism (MCD), variable temperature
130 DHBD, EC 1.13.11.39), has been studied using magnetic circular dichroism (MCD), variable-temperature
131 roscopy, we have used electronic absorption, magnetic circular dichroism (MCD), variable-temperature,
133 , to our knowledge, the first tabletop X-ray magnetic circular dichroism measurements at the N4,5 abs
134 ic spectrum, and use them to implement X-ray magnetic circular dichroism measurements in a tabletop-s
138 ucting quantum interference device and X-ray magnetic circular dichroism measurements, we observe cle
140 n (mu-XRD) using a focused X-ray beam, X-ray Magnetic Circular Dichroism - Photo Emission Electron Mi
141 characteristic feature of NI is the intense magnetic circular dichroism pseudo-A feature (a pair of
142 use diffuse reflectance UV-vis spectroscopy, magnetic circular dichroism, resonance Raman spectroscop
143 utagenesis, ligand-binding measurements, and magnetic circular dichroism, resonance Raman, and electr
144 Detailed low-temperature absorption and magnetic circular dichroism, resonance Raman, and electr
146 -temperature absorption, circular dichroism, magnetic circular dichroism, resonance Raman, EPR and X-
147 UV-visible absorption, variable temperature magnetic circular dichroism, resonance Raman, Mossbauer,
150 ed hysteresis loop emerges in the reflective magnetic circular dichroism signal as a function of magn
154 rption, electron paramagnetic resonance, and magnetic circular dichroism spectra of these variants pr
155 rbance, electron paramagnetic resonance, and magnetic circular dichroism spectra showed a high spin f
156 53 nm, shoulder at approximately 585 nm) and magnetic circular dichroism spectra that are nearly iden
157 ibe detailed time-resolved mass spectral and magnetic circular dichroism spectral data recorded as he
158 sm, and variable-temperature, variable-field magnetic circular dichroism spectroscopic experiments ha
160 In the present study, in situ Mossbauer and magnetic circular dichroism spectroscopic studies combin
162 resonance (EPR), electronic absorption, and magnetic circular dichroism spectroscopies have been per
167 etical framework developed by solution-state magnetic circular dichroism spectroscopists: the Faraday
168 e cofactor were monitored with time-resolved magnetic circular dichroism spectroscopy after photodiss
169 enomena, resonance Raman data are coupled to magnetic circular dichroism spectroscopy and density fun
171 s by experimental X-ray absorption and X-ray magnetic circular dichroism spectroscopy combined with m
172 e for a methyl-Ni(III) species; furthermore, magnetic circular dichroism spectroscopy identified the
175 ined by variable-temperature, variable-field magnetic circular dichroism spectroscopy on a previously
176 UV-visible absorption, resonance Raman, and magnetic circular dichroism spectroscopy that Cu(A)CcP i
177 we use variable-temperature, variable-field magnetic circular dichroism spectroscopy to define the g
179 ar structure differences, Mossbauer spectra, magnetic circular dichroism spectroscopy, and integer-sp
180 raction, electronic absorption spectroscopy, magnetic circular dichroism spectroscopy, magnetic susce
181 ion, and variable temperature/variable field magnetic circular dichroism spectroscopy, provide strong
182 mechanism is systematically investigated by magnetic circular dichroism spectroscopy, ultrafast tran
187 Resonance Raman and variable-temperature magnetic circular dichroism studies of heme-free prepara
192 ctroscopy, X-ray linear dichroism, and X-ray magnetic circular dichroism study, combined with density
193 n of these systems on surfaces, ranging from magnetic circular dichroism to magnetic force microscopy
196 anced X-ray techniques are applied, based on magnetic circular dichroism, to investigate the spin tex
197 ant, but its lifetime agrees with a reported magnetic circular dichroism transient, which has been at
198 esized and studied by electronic absorption, magnetic circular dichroism, transmission electron micro
199 d using a combination of circular dichroism, magnetic circular dichroism, variable-temperature variab
201 n of UV/visible/near-IR variable-temperature magnetic circular dichroism (VTMCD) and EPR spectroscopi
202 zed protein and EPR and variable-temperature magnetic circular dichroism (VTMCD) studies of the as-pr
203 the combination of EPR, variable-temperature magnetic circular dichroism (VTMCD), and resonance Raman
204 -visible absorption and variable-temperature magnetic circular dichroism (VTMCD), EPR, and resonance
205 /NIR absorption, CD and variable-temperature magnetic circular dichroism (VTMCD), EPR, and X-ray abso
206 ation of variable-temperature variable-field magnetic circular dichroism (VTVH MCD) and powder/single
207 AS), and variable-temperature-variable-field magnetic circular dichroism (VTVH MCD) spectroscopy, we
208 e, using variable-temperature variable field magnetic circular dichroism (VTVH MCD) spectroscopy.
209 tein, a variable-temperature, variable-field magnetic circular dichroism (VTVH-MCD) spectroscopic stu
212 ts, X-ray absorption spectroscopy, and X-ray magnetic circular dichroism, we have determined the natu
213 der of magnetic octupole in Mn(3)Sn by X-ray magnetic circular dichroism, which is only predicted the
214 r characterization by electronic absorption, magnetic circular dichroism, X-ray absorption, magnetic
215 N@C(80) endofullerene was studied with X-ray magnetic circular dichroism (XMCD) and a magnetometer wi
216 xial Fe/graphene interface by means of X-ray magnetic circular dichroism (XMCD) and density functiona
222 rough X-ray linear dichroism (XLD) and X-ray magnetic circular dichroism (XMCD) measurements, further
224 ributions, as established by combining X-ray magnetic circular dichroism (XMCD) spectroscopy and bulk
225 erein, we present Fe and Mo L(3) -edge X-ray magnetic circular dichroism (XMCD) spectroscopy of the (
228 , x-ray absorption spectroscopy (XAS), x-ray magnetic circular dichroism (XMCD), and specular/off-spe
229 based microscopy techniques [including X-ray magnetic circular dichroism (XMCD)] reveals that symbion