ライフサイエンスコーパス: field dependence

1 m temperature resistance, appears to lack MR field dependence.

2 resistivity data showed a nonlinear magnetic field dependence.

3 e microparticles under two distinct electric field dependences.

4 ence of the Kondo resonance and its magnetic field dependence agree with a simple interpretation of t

5 via transport measurement and their magnetic field dependence agrees with the theoretical expectation

6 single type of 15N-coupled nucleus from the field dependence, along with the absence of an associate

7 lains simultaneously the frequency (magnetic field) dependence and the angular anisotropy of the rela

8 l electric polarization, its strong magnetic field dependence, and the negative thermal expansion in

9 racter split into two peaks with an X-shaped field dependence as a clear fingerprint of the shift of

10 characteristic spin selectivity and magnetic field dependence, being the model also for more complica

11 measured, and the inverse square law of the field dependence can be determined quantitatively.

12 wn mechanisms can explain the observed sharp field dependence, fast breakdown times and observed surf

13 When the slope of the electric field dependence goes to 0 as r goes to infinity and 1/r

14 In addition, the lack of electric field dependence in the charge dynamics rules out gemina

15 pling constants (J(HN) and J(HH)) and of the field dependence in the formation of the observed (15)N

16 ncluding the effects of optical aberrations, field dependence in the imaging system, fluorophore labe

17 al resistivity rhoxx shows a linear magnetic field dependence in the quantum limit regime.

18 me of reference to perceive vertical (visual field dependence-independence perceptual style).

19 The magnetic field-dependence indicates that the chemical exchange br

20 endence of free-carrier generation, and this field dependence is considerably weaker compared to that

21 ed for thickness the current versus electric field dependence is indistinguishable.

22 The slope of the electric field dependence is inversely related to the molecular r

23 ature, optical excitation power and electric-field-dependence measurements demonstrate that the quenc

24 Measurements of the temperature and magnetic field dependence of a Coulomb-blockaded dot show good ag

25 The field dependence of ABS manifests a substantially enhanc

26 iltonian accurately predicts temperature and field dependence of both magnetic structure and magnetiz

27 e measure the quantum yield and the electric field dependence of charge generation on excitation of t

28 he densities of donor states and predict the field dependence of charge transfer in excellent agreeme

29 Combined with the magnetic field dependence of chi(kagome) that we observed at low

30 lish a systematic framework for the magnetic field dependence of electrostatically gated quantum spin

31 sight into the effect of fluorination on the field dependence of free charge-carrier generation and r

32 T is shown to exhibit a significantly weaker field dependence of free charge-carrier generation combi

33 T with PC(70)BM is largely determined by the field dependence of free-carrier generation, and this fi

34 The latter is evaluated from the magnetic field dependence of Gamma(1) in conjunction with Gamma(2

35 This field dependence of inductance arises from the change of

36 The in-plane magnetic field dependence of interlayer critical current, togethe

37 rom characteristic dispersion curves or from field dependence of ion mobility was experimentally demo

38 by low-field ion mobility and exploiting the field dependence of ion mobility, potentially allowing s

39 The field dependence of ions, described as an alpha paramete

40 The magnetic-field dependence of k+/- of the triads with phenylene br

41 We exploit the temperature and magnetic field dependence of magnetic entropy change (DeltaS M) t

42 the composite changes substantially and the field dependence of magnetization reveals ferromagnetic-

43 lectivity in response through differences in field dependence of mobility for ions in purified air at

44 d approximation of errors resulting from the field dependence of optical aberrations.

45 nse, that the heterostructure shows magnetic field dependence of piezoelectricity due to the improved

46 lobal analysis of the temperature and static field dependence of R(ex)(1/tau(cp)) for Cys 14 and Lys

47 ads to a pronounced temperature and magnetic field dependence of radiative decay.

48 xtracted from (31)P relaxation rates and the field dependence of relaxation rates for several protons

49 We map the magnetic-field dependence of spin-wave excitations by detecting t

50 The field dependence of STM images and point I-V curves indi

51 The magnetic field dependence of the 31P spin-lattice relaxation rate

52 orption data published earlier; the magnetic field dependence of the amplitude of this kinetic compon

53 r the measurement of RDCs using the magnetic-field dependence of the apparent one-bond 1H-15N J coupl

54 Measurement of the in-plane magnetic field dependence of the chemical potential near filling

55 , we find a correlation between the magnetic field dependence of the conductivity and the helicity of

56 The magnitude and field dependence of the critical current are related to

57 We report the magnetic field dependence of the critical solidification rate for

58 ce of defects, the intrinsic temperature and field dependence of the domain-wall velocity can be desc

59 econcile recent contradicting reports of the field dependence of the droplet nucleation.

60 The temperature and magnetic-field dependence of the electrical resistivity and speci

61 he observed temperature, power, and magnetic-field dependence of the exciton density.

62 We propose that the anomalous field dependence of the form factor arises from Pauli pa

63 ignificantly alter the frequencies, magnetic field dependence of the frequencies, and the power and p

64 harp, current-sensitive peak in the magnetic field dependence of the Hall resistivity, and (2) A curr

65 ound in calcium-exchanged zeolites where the field dependence of the line width indicates a distribut

66 Magnetic ordering was reflected in a field dependence of the magnetic susceptibility below 3.

67 The field dependence of the magnetization, M(H), at 2 K for

68 By mapping the external field dependence of the measured resonance frequency, we

69 ussed based on the frequency, viscosity, and field dependence of the observed trapping force.

70 The magnetic field dependence of the paramagnetic contributions in bo

71 hertz was revealed by a peak in the magnetic field dependence of the proton spin-lattice relaxation r

72 e have extended measurements of the magnetic field dependence of the proton-spin-lattice-relaxation r

73 Here, we present systematic magnetic field dependence of the proximity effect in Au/SrRuO(3)/

74 The dc-field dependence of the relaxation time was studied to r

75 ed an anomalous and unprecedentedly observed field dependence of the relaxation time, which was model

76 We explore the magnetic field dependence of the SABRE-Relay efficiency and show

77 ever, the voltage, temperature, and magnetic field dependence of the signals agree with predictions f

78 The electric field dependence of the single-dot spectrum is character

79 general study of the frequency and magnetic field dependence of the specific heat power produced dur

80 transition proposed recently to explain the field dependence of the spin cluster dynamics.

81 hoinositide (31)P linewidths and on the full field dependence of the spin-lattice relaxation rate (me

82 Here, we report the pressure and magnetic field dependence of the superconducting order observed i

83 The magnetic field dependence of the superconductivity in nanocrystal

84 Some field dependence of the susceptibility below 3 K is obse

85 in-wave theory and conclude that the unusual field dependence of the transition temperature is a hall

86 The phase and magnetic-field dependence of the zero-energy states is consistent

87 The temperature and magnetic field dependence of these oscillations yields crucial in

88 strain and phonon anharmonicity explains the field dependence of v(LA), kappa, and D without any adju

89 experiments on the temperature and magnetic field dependences of AHE in insulating, strongly-disorde

90 y by the unique carrier-density and magnetic-field dependences of different moire exciton resonances.

91 We find that the temperature and magnetic field dependences of the resistivity of LNO at low tempe

92 om electrophoretic movement of DNA in the ac field, dependence of the DNA/membrane interaction on the

93 From the results of THz pump field dependence, pump/probe polarization dependence, an

94 Magnetic field dependence reveals a fluctuating exchange splittin

95 lifetime, transient absorption, and magnetic field dependence studies.

96 At the microscopic level, based on the field dependence theory of magnetic disorder in scattere

97 e extrapolation of the slope of the electric field dependence to zero electric field can be used to e

98 and their aggregates display clear magnetic field dependences up to 25 T, with the aggregates showin

99 measuring the temperature and magnetic bias field dependences, where the X-ray magnetic linear dichr

100 r Hall conductivity has a nonlinear magnetic field dependence, which can be attributed to the magneti

101 T (MI) demonstrates anisotropic magnetic field dependence with the preferred orientation along th

102 gnetic relaxation time shows a pronounced dc-field dependence, with a maximum occurring at approximat