ライフサイエンスコーパス: magnetometry

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

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

3 acroscopic ferromagnetism was found in SQUID magnetometry.

4 tomic-scale spin centres for sensitive local magnetometry.

5 cular dichroism (MCD) spectroscopy and SQUID magnetometry.

6 and the magnetic anomaly observed in torque magnetometry.

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

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

9 o investigated by NIR spectroscopy and SQUID magnetometry.

10 cting magnets and cryogenics: optical atomic magnetometry.

11 y transmission electron microscopy and SQUID magnetometry.

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

13 , 6Li MAS NMR, electron microscopy (EM), and magnetometry.

14 confirmed by X-ray crystallography and SQUID magnetometry.

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

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

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

18 Quasi-static magnetometry and dynamic ferromagnetic resonance measure

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

20 Squid magnetometry and EPR studies yield data that are consist

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

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

23 Magnetometry and low-temperature ND experiments show tha

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

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

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

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

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

29 11-13), respectively, as determined by SQUID magnetometry and numerical fits to linear combinations o

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

31 Our magnetometry and structural measurements show that a per

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

48 Magnetometry experiments show a strong, adjustable diama

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

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

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

52 Although solid-state magnetometry indicates an antiferromagnetic interaction

53 SQUID magnetometry indicates hysteresis below 6 K, while therm

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

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

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

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

58 SQUID magnetometry measurements indicate that 5 is a macromole

59 We present cantilever magnetometry measurements performed on mesoscopic sample

60 SQUID magnetometry measurements showed a single-crystal sample

61 Magnetometry measurements suggest changes in the microst

62 magnetic field sequence and demonstrated in magnetometry measurements.

63 elate with values obtained in separate SQUID magnetometry measurements.

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

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

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

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

68 Mossbauer spectroscopy and magnetometry reveal strong magnetic interactions within

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

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

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

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

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

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

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

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

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

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

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

80 SQUID magnetometry suggests that the iron containing samples a

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

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

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

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

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

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

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

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

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

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

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

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