ライフサイエンスコーパス: magnetometry

1 iltering technique (i.e., synthetic aperture magnetometry).

2 nfrared spectroscopy (DRIFT), XPS, and SQUID magnetometry.

3 o investigated by NIR spectroscopy and SQUID magnetometry.

4 cting magnets and cryogenics: optical atomic magnetometry.

5 y transmission electron microscopy and SQUID magnetometry.

6 enced by XRD, NEXAFS spectroscopy, and SQUID magnetometry.

7 , 6Li MAS NMR, electron microscopy (EM), and magnetometry.

8 ion analysis, UV-vis spectroscopy, and SQUID magnetometry.

9 ver and use it to demonstrate scanning probe magnetometry.

10 e experimentally demonstrate laser threshold magnetometry.

11 ying our protocol to quantum enhanced atomic magnetometry.

12 nducting quantum interference device (SQUID) magnetometry.

13 laser methods offer improved sensitivity for magnetometry.

14 or development toward coherent approaches to magnetometry.

15 re continuous wave EPR experiments and SQUID magnetometry.

16 t with the largely diamagnetic response from magnetometry.

17 toelectron spectroscopy and vibrating sample magnetometry.

18 erpolarization methods with state-of-the-art magnetometry.

19 -1), as determined by EPR spectroscopy/SQUID magnetometry.

20 irmed by electron paramagnetic resonance and magnetometry.

21 ermally active ASI systems by means of SQUID magnetometry.

22 tomic-scale spin centres for sensitive local magnetometry.

23 confirmed by X-ray crystallography and SQUID magnetometry.

24 ng an S = 2 spin state as confirmed by SQUID magnetometry.

25 = 5.8 K) already evidenced by direct current magnetometry.

26 acroscopic ferromagnetism was found in SQUID magnetometry.

27 elated with the increase in T(C) measured by magnetometry.

28 cular dichroism (MCD) spectroscopy and SQUID magnetometry.

29 and the magnetic anomaly observed in torque magnetometry.

30 properties of 1-3 were investigated by SQUID magnetometry.

31 ology(1), quantum information processing(2), magnetometry(3) and precision tests of the standard mode

32 terized by X-ray diffraction analysis, SQUID magnetometry, (57)Fe Mossbauer spectroscopy, and cyclic

33 roscopy (TEM) and alternative gradient force magnetometry (AGFM) clearly demonstrate the successful a

34 g with EDX analysis, XPS analysis, and SQUID magnetometry analysis of catalytic solutions.

35 mentally characterized by a vibrating sample magnetometry and a frequency-swept ferromagnetic resonan

36 ation processes dominate, as demonstrated by magnetometry and ab initio computational methods.

37 Both SQUID magnetometry and broken-symmetry DFT computations reveal

38 rystallography, UV/vis and EPR spectroscopy, magnetometry and computational methods reveal that the r

39 Heat capacity, magnetometry and direct adiabatic temperature change mea

40 Quasi-static magnetometry and dynamic ferromagnetic resonance measure

41 By performing simultaneous magnetometry and electrical transport measurements, we o

42 excited states are detectable both by SQUID magnetometry and electron paramagnetic resonance (EPR) s

43 ier of approximately 8 K, determined by bulk magnetometry and electron paramagnetic resonance.

44 anisotropic structure is studied in depth by magnetometry and electron spin resonance.

45 SQUID magnetometry and EPR spectroscopy suggest that the Sb(2)

46 SCF-SO calculations and confirmed with SQUID magnetometry and EPR spectroscopy, showing easy-axis or

47 S = 3/2, ground state, as confirmed by SQUID magnetometry and EPR spectroscopy.

48 Squid magnetometry and EPR studies yield data that are consist

49 nge coupling, Aex, is determined using SQUID magnetometry and ferromagnetic resonance (FMR), displayi

50 = (9)/(2) spin state as determined by SQUID magnetometry and further supported by quantum chemical c

51 Variable-temperature SQUID magnetometry and IR, NIR, and EPR spectroscopies on the

52 d metasurface is very promising for sensing, magnetometry and light modulation applications.

53 Magnetometry and low-temperature ND experiments show tha

54 By combining micromanipulation, Kerr magnetometry and magnetic force microscopy, we determine

55 It is shown by magnetometry and microSR spectroscopy that short-range m

56 Using a combination of magnetometry and muon spin relaxation measurements, we d

57 re using neutron powder diffraction and used magnetometry and muon-spin rotation data to determine th

58 y x-ray diffraction, transport measurements, magnetometry and neutron diffraction.

59 11-13), respectively, as determined by SQUID magnetometry and numerical fits to linear combinations o

60 Spacecraft magnetometry and paleomagnetic measurements of lunar sam

61 s investigated using field-cooling-dependent magnetometry and polarized neutron reflectometry.

62 properties have been characterized via SQUID magnetometry and Raman spectroscopy.

63 ng so rapidly that conventional methods like magnetometry and SC-XRD are unable to detect it.

64 alt(II) complex, studied by a combination of magnetometry and spectroscopy.

65 Our magnetometry and structural measurements show that a per

66 Using SQUID magnetometry and X-ray absorption spectroscopy, we demon

67 tering, superconducting quantum interference magnetometry, and atomic force microscopy.

68 for example, quantum technologies, nanoscale magnetometry, and biosensing.

69 ent films also enable advanced spectroscopy, magnetometry, and cavity magnonic measurements that reve

70 ctronic and X-ray absorption spectroscopies, magnetometry, and computational analyses.

71 dence from single-crystal X-ray diffraction, magnetometry, and computational techniques, the slow spi

72 id state structure, UV-visible spectroscopy, magnetometry, and cyclic voltammetry data along with the

73 roscopy, X-ray diffraction, vibrating sample magnetometry, and cyclic voltammetry.

74 al X-ray diffraction analyses, spectroscopy, magnetometry, and Density Functional Theory (DFT) calcul

75 EPR spectroscopy, SQUID magnetometry, and DFT calculations thoroughly characteri

76 on, electron microscopy, Raman spectroscopy, magnetometry, and electrical transport measurements.

77 , crystal structure, electrochemistry, SQUID magnetometry, and EPR spectroscopy of a Mn(III)Mn(IV)(3)

78 superconducting quantum interference device magnetometry, and in vitro magnetic needle extraction we

79 st properties were measured using 64 mT MRI, magnetometry, and nuclear magnetic resonance dispersion

80 superconducting quantum interference device magnetometry, and one (8+) by nuclear magnetic resonance

81 ermined by EPR, zero-field (57)Fe Mossbauer, magnetometry, and single crystal X-ray diffraction.

82 haracterised through EPR spectroscopy, SQUID magnetometry, and supporting computational analysis, whi

83 tructure theory, nuclear magnetic resonance, magnetometry, and terahertz electron paramagnetic resona

84 aphy, field, temperature, and time-dependent magnetometry, and the application of a new magnetization

85 fraction, UV-vis and EPR spectroscopy, SQUID magnetometry, and theoretical computations.

86 Mossbauer spectroscopy, magnetometry, and variable-temperature neutron diffracti

87 electronic absorption spectroscopies, SQUID magnetometry, and X-ray crystallography.

88 ssbauer spectroscopy, (1)H NMR spectroscopy, magnetometry, and X-ray diffraction.

89 Magnetometry- and EPR-related results are tabulated and

90 Here we introduce single-spin magnetometry as a generic platform for nonperturbative,

91 highlights scanning nitrogen-vacancy center magnetometry as a quantitative probe to explore nanoscal

92 Our results establish color center magnetometry as a versatile tool for advancing spin-wave

93 te our findings with an example of NV-centre magnetometry, as well as schemes involving spin-1/2 prob

94 r Nd(2)GaMnO(6) formula unit was measured by magnetometry at 5 K in an applied magnetic field of 5 T.

95 eing the ideal candidate for ultra-sensitive magnetometry at ambient conditions without any optical c

96 adigm of indirect encoding for vector atomic magnetometry based on machine learning.

97 tical approach to meet this challenge, using magnetometry based on single nitrogen-vacancy centres in

98 irst order reversal curve (FORC) method is a magnetometry based technique used to capture nanoscale m

99 ces were localized with a synthetic aperture magnetometry beamforming analysis of visually cued index

100 ntiferromagnetic behavior, confirmed by bulk magnetometry characterizations.

101 nducting quantum interference device (SQUID) magnetometry confirmed and quantitatively characterized

102 diffraction (PXRD), UV-Vis spectroscopy, and magnetometry confirmed Fe(3)O(4)-based nanomaterial form

103 Mossbauer, NMR, and EPR spectroscopies with magnetometry, crystallography, and advanced theoretical

104 Combining cantilever torque magnetometry data with ab initio calculations allowed us

105 ar-infrared (UV-vis/NIR) spectroscopy, SQUID magnetometry, DFT and multiconfigurational ab initio cal

106 nducting quantum interference device (SQUID) magnetometry, double-coil mutual inductance, and magneto

107 abeling, electronic absorption spectroscopy, magnetometry, electronic structure calculations, element

108 rized, including by X-ray diffraction, SQUID magnetometry, EPR and XAS/XES spectroscopies, and DFT ca

109 superconducting quantum interference device magnetometry, EPR spectroscopy in various matrices, and

110 erized by X-ray crystallography, while SQUID magnetometry, EPR spectroscopy, and UV-vis-NIR spectrosc

111 Magnetometry experiments show a strong, adjustable diama

112 antiferromagnetic interactions evaluated by magnetometry experiments.

113 core/shell nanoparticles is demonstrated by magnetometry, ferromagnetic resonance and X-ray magnetic

114 We report results from SQUID magnetometry, ferromagnetic resonance as well as Brillou

115 [Formula: see text] cannot be observed in DC magnetometry for low temperature baked niobium unlike fo

116 Furthermore, SQUID magnetometry from 5 to 300 K of solid [(+)-NDI-Delta(3(-

117 Using magnetometry, heat capacity, and electron paramagnetic r

118 nducting Quantum Interference Device (SQUID) magnetometry, high-field electron paramagnetic resonance

119 display the capability of capacitive torque magnetometry in characterizing the magneto-chemical pote

120 ed a monomeric Bi(II) structure, while SQUID magnetometry in combination with NMR and EPR spectroscop

121 c properties of 3 are characterized by SQUID magnetometry in polystyrene glass and by quantitative EP

122 ternally applied magnetic field to enable dc magnetometry in solution.

123 tion and Mossbauer spectroscopies, and SQUID magnetometry indicate that there are tetrahedral high-sp

124 Volume magnetometry indicates [Formula: see text] K with a magn

125 Although solid-state magnetometry indicates an antiferromagnetic interaction

126 SQUID magnetometry indicates hysteresis below 6 K, while therm

127 we demonstrate the ability to perform local magnetometry inside a diamond anvil cell with sub-micron

128 Magnetometry is a powerful tool for fathoming electrons

129 Color center magnetometry is a promising tool for imaging spin waves,

130 NV diamond magnetometry is noninvasive and label-free and does not

131 Cantilever torque magnetometry is used to elucidate the orientation of mag

132 nduced magnetization is easily measurable by magnetometry, low-energy muon spin spectroscopy provides

133 ate was characterized using vibrating sample magnetometry, magnetic force microscopy, and MRI.

134 g possibilities in fluorescent protein-based magnetometry, magnetic imaging, and magnetogenetic contr

135 nducting quantum interference device (SQUID) magnetometry, magneto-absorption and transient optical s

136 iffraction analysis, (57)Fe Mossbauer, SQUID magnetometry, mass spectrometry, and combustion analysis

137 In the future, magnetometry may be used to study long-distance electric

138 SQUID magnetometry measurements indicate that 5 is a macromole

139 ent removal causes decomposition of the MOF, magnetometry measurements of the MOF containing only N-o

140 Angular magnetometry measurements performed on a single crystal

141 We present cantilever magnetometry measurements performed on mesoscopic sample

142 SQUID magnetometry measurements showed a single-crystal sample

143 Magnetometry measurements suggest changes in the microst

144 However, local magnetometry measurements under high pressure still rema

145 elate with values obtained in separate SQUID magnetometry measurements.

146 magnetic field sequence and demonstrated in magnetometry measurements.

147 Magnetometry, Mossbauer and Raman spectroscopy confirm t

148 SQUID magnetometry, Mossbauer spectroscopy, and DFT calculatio

149 lous scattering studies, cyclic voltammetry, magnetometry, Mossbauer spectroscopy, UV-vis-NIR spectro

150 Magnetometry, neutron scattering, and calorimetry are us

151 al and theoretical techniques, such as SQUID magnetometry of polycrystalline powders, EPR spectroscop

152 pared diradical 1 are characterized by SQUID magnetometry of polycrystalline powders, in polystyrene

153 thermodynamic signatures, observed by torque magnetometry, of bosonic LL transitions in the layered s

154 Multiparameter sensing such as vector magnetometry often involves complex setups due to variou

155 gh stroboscopic neutron scattering and SQUID magnetometry on a new class of ultrapure Ho(2)Ti(2)O(7)

156 In addition, vector magnetometry on the driving fields reveals contributions

157 ed spectroscopy (fNIRS) and optically pumped magnetometry (OPM), and innovative applications of funct

158 electronic structure of this 5f(1) family by magnetometry, optical and electron paramagnetic resonanc

159 f D = +7.95 or +9.2 cm(-1), as determined by magnetometry or electron paramagnetic resonance spectros

160 Taking advantage of a scanning single-spin magnetometry platform, here we report observation of two

161 e results demonstrate that cantilever torque magnetometry provides a powerful route to characterize t

162 This demonstrates that torque magnetometry provides a sensitive test for J(eff) and th

163 electronic spin in diamond, composite-pulse magnetometry provides a tunable trade-off between sensit

164 Scanning single-spin and wide-field magnetometry reveal a parabolic Poiseuille profile for e

165 Mossbauer spectroscopy and magnetometry reveal strong magnetic interactions within

166 s investigated by variable-temperature SQUID magnetometry, reveal weak intramolecular antiferromagnet

167 nducting quantum interference device (SQUID) magnetometry revealing a one-dimensional S = 1/2 antifer

168 vestigated by alternating current (ac) SQUID magnetometry, revealing slow magnetic relaxation in both

169 DC SQUID magnetometry reveals Curie-Weiss behavior for T > 20 K (

170 Continuous but nondestructive magnetometry reveals previously unseen spin dynamics, fi

171 SQUID magnetometry reveals that 1 has an effective barrier to

172 sis was completed using a synthetic aperture magnetometry (SAM) technique, while the fMRI data were a

173 pulse known as rotary-echo yields a flexible magnetometry scheme, mitigating both driving power imper

174 ser-based readout applied to near zero-field magnetometry showcases the measurement signal-to-noise r

175 terized by EPR, zero-field (57)Fe Mossbauer, magnetometry, single crystal X-ray diffraction, XAS, and

176 tem Sr2MgOsO6 is probed via a combination of magnetometry, specific heat measurements, elastic and in

177 )Pr2P(Se)NP(Se)(i)Pr2}2] was investigated by magnetometry, spectroscopic, and quantum chemical method

178 Combined magnetometry, spin resolved inverse photoemission, elect

179 From the combination of magnetometry, spin-polarized photoemission spectroscopy,

180 Angle-resolved magnetometry studies revealed the orientation of the mag

181 Magnetometry studies showed that V{N(H)Ar(iPr6)}2 and V{

182 t single-crystal X-ray diffraction and SQUID magnetometry suggest a Np(III) -U(VI) assignment.

183 ESR, NMR, and magnetometry suggest both species have singlet ground st

184 SQUID magnetometry suggests that the iron containing samples a

185 X-ray photoelectron spectroscopy, EPR, and magnetometry support this assignment.

186 superconducting quantum interference device magnetometry, surface-sensitive X-ray magnetic circular

187 Using four complementary magnetometry techniques and theoretical simulations, a r

188 Laser threshold magnetometry theory predicts improved NV center ensemble

189 physical observations of LiNiO(2), including magnetometry, thermally activated electronic conduction,

190 imental and theoretical approaches including magnetometry, thermodynamic measurements, neutron scatte

191 ption, as well as EPR spectroscopy and SQUID magnetometry, thus confirming the C(S) symmetry and the

192 symmetric graph state resources for quantum magnetometry to enhance measurement precision by analyzi

193 photoelectron spectroscopy (XPS), and SQUID magnetometry to gain information on its morphological, c

194 Here, we leverage atomic magnetometry to map the weak induced magnetic fields aro

195 We use torque magnetometry to measure the magnetic response of NbP up

196 As a second example, we apply magnetometry to observe the chemical-exchange-driven (13

197 Here we use differential magnetometry to probe spin rotation in the 3D topologica

198 In this study, we employed cantilever torque magnetometry to probe the magnetic anisotropy of a singl

199 Here we use single spin magnetometry to quantitatively characterise saturation m

200 fashion and offers the possibility of using magnetometry to report host-guest interactions.

201 We used torque magnetometry to resolve the Fermi surface topology in th

202 We employ in situ optical magnetometry to sensitively detect and characterize the

203 re, we employ scanning nitrogen vacancy (NV) magnetometry to unveil the morphogenesis of spin cycloid

204 a uniquely versatile platform for nanoscale magnetometry under diverse environmental conditions.

205 Here, we develop SQUID magnetometry under extreme high-pressure conditions and

206 isostructural compound and milikelvin torque magnetometry unravels the role of the single-molecule an

207 Here, we employ cryogenic scanning magnetometry using a single-electron spin of a nitrogen-

208 ntary techniques, including vibrating-sample magnetometry (VSM), energy-dispersive X-ray spectroscopy

209 ), X-ray diffraction (XRD), vibrating sample magnetometry (VSM), inductively coupled plasma (ICP) ato

210 Using time resolved magnetometry we show that the relaxation process can be

211 combination of neutron diffraction and bulk magnetometry we show that these materials are noncolline

212 Using single-spin quantum magnetometry, we directly visualized nanoscale magnetic

213 By using torque magnetometry, we have investigated the magnetization of

214 Using nitrogen vacancy-based diamond magnetometry, we observe the magnetic spin cycloid struc

215 Applying this technique to magnetometry, we show magnetic sensitivity approaching t

216 spatially resolving nitrogen-vacancy center magnetometry, we show that Fe:MoS(2) monolayers remain m

217 Using local magnetometry, we show that superconductivity straddles a

218 nic absorption spectroscopy as well as SQUID magnetometry, which all confirmed the electronic structu

219 roperties of 1-4 have been assessed by SQUID magnetometry, while a DFT analysis of complexes 1 and 6

220 erized using (1)H NMR spectroscopy and SQUID magnetometry, while all species were structurally charac

221 magnet, its combination with optical atomic magnetometry will greatly broaden the analytical capabil

222 -temperature zero-field (57)Fe Mossbauer and magnetometry with a spin reversal barrier of 42.5(8) cm(

223 pectroscopy (XPS), FT-IR spectroscopy, SQUID magnetometry, X-ray absorption fine structure (XAFS), an