ライフサイエンスコーパス: gauss

1 m core field strength of approximately 10(7) gauss.

2 1.05 to 1.35 solar radii, are mostly 1 to 4 gauss.

3 face magnetic fields, B approximately 10(15) gauss.

4 nos, and magnetic fields in excess of 10(13) Gauss.

5 5 and 1.60 solar radii varies from <1 to ~20 gauss.

6 ely strong magnetic fields (10(13) to 10(15) gauss)(1,2), which episodically emit X-ray bursts approx

7 The GAUSS-2 (Goal Achievement after Utilizing an Anti-PCSK9

8 reconstituted with the human btk gene to a 1-gauss 60-Hz electromagnetic field (EMF) has been reporte

9 support the hypothesis that exposure to a 1-gauss 60-Hz EMF had a causal effect on protein-tyrosine

10 control, showed no significant effect of a 1-gauss 60-Hz EMF on Ins 1,4,5-P3 production.

11 t analysis Association Using Sparse Signals (GAUSS), a method for gene set association analysis that

12 nt Genome Analysis Using Summary Statistics (GAUSS)-a comprehensive and user-friendly R package desig

13 white dwarf in MV Lyrae of between 2 x 10(4) gauss and 1 x 10(5) gauss, too low to be detectable by o

14 gle line with a peak-to-peak linewidth of 15 Gauss and a g value of 2.0035.

15 magnetar-strength magnetic fields (of 10(15) gauss and above) and for powering the explosion of a rot

16 ge modal fidelity above 80% for 210 Laguerre-Gauss and Hermite-Gauss modes by using vectorial time re

17 Starting with Gauss and Kelvin, knots in fields were postulated to beh

18 Expressions are given for the Gauss and Mean curvatures of a surface of thickness h.

19 .6, comparable to the second-harmonic Bessel Gauss beam, and 2.8 x the value obtained for the second-

20 Gaussian wave packet, Airy beam, and Bessel Gauss beam.

21 n that of the Gaussian, Airy beam and Bessel Gauss beams, respectively, demonstrating a strong correl

22 uced defects always obeys predictions of the Gauss-Bonnet and Poincare-Hopf index theorems.

23 Motivated by the Gauss-Bonnet theorem that correlates the geodesic curvat

24 traints must be satisfied, namely the famous Gauss-Bonnet theorem, and an inequality stemming from th

25 r closed surfaces, a quantum analogue of the Gauss-Bonnet theorem.

26 , scalar and matter fields in context of the Gauss-Bonnet theories.

27 emely high magnetic fields (10(14) to 10(15) gauss), called magnetars(1,3,4).

28 in the electronic absorption spectra and < 8 gauss changes in the copper hyperfine coupling constants

29 re using the Second Fundamental Form and the Gauss-Codazzi equation.

30 scale has been detected to date (<2 x 10(21) Gauss-cubic centimeter), but here the discovery of multi

31 generated by a conflict between the positive Gauss curvature of the assembling capsid and the negativ

32 re of the assembling capsid and the negative Gauss curvature of the neck region.

33 In contrast, for surfaces with negative Gauss curvature the surface deforms nonlocally along cha

34 find that for surfaces with zero or positive Gauss curvature, a common feature of the response is the

35 represented by new high-dimensional features-Gauss curvature-based coordinates.

36 which turn into surface-like information via Gauss curvatures.

37 gnetic field strength is high (a few hundred Gauss), develops the SEP composition signature.

38 This paper shows that, by Gauss divergence theorem, the gravitational force inside

39 ng proportions of causal genes, we find that GAUSS effectively controls type 1 error rate and has gre

40 As a result, GAUSS elevates the quality and applicability of existing

41 uss in small external fields (less than 1000 gauss), enabling ferromagnetic control of local electron

42 theory show that single atoms synthesized by GAUSS enhance the lithium-sulfur redox reaction kinetics

43 Gauss et al. present evidence that an endoplasmic reticu

44 The Gauss-Euler elastica underlies a theoretical framework t

45 governed by a principle, which we call the "Gauss-Euler elastica" This emergent rule states that-des

46 shbach resonances, of the order of three per gauss for bosons.

47 ical with an overall EPR line width of 29-31 gauss (G) was generated by reaction of PGHS-2 with ethyl

48 uced tyrosyl radical from a functional 33-35-gauss (G) wide doublet/wide singlet to a 26-G narrow sin

49 Applying a Gauss-Hermite filter reduced noise in the extinction spe

50 uncation in the meriodonal direction through Gauss--Hermite quadrature projected onto a simple discre

51 beams, which can be transformed into Hermite-Gauss (HG) beams through astigmatic transformations usin

52 For each significantly associated gene set, GAUSS identifies the subset of genes that have the maxim

53 sulting hyperfine fields are as high as 9000 gauss in small external fields (less than 1000 gauss), e

54 We found that GAUSS is scalable and identified 13,466 phenotype and ge

55 expressions are suggested to determine both Gauss (K) and Mean (H) curvatures as functions of invari

56 ial differential equations (Ampere's law and Gauss' law for magnetism) numerically with the aid of ph

57 vection-diffusion equation coupled either to Gauss' law or Poisson's equation, depending on the choic

58 d light carrying OAM states include Laguerre-Gauss (LG) beams, which can be transformed into Hermite-

59 In this work, we show how to use the Gauss linking integral (GLN) in the form of a matrix dia

60 By employing mathematical topology metrics (Gauss linking integral, writhe and second Vassiliev meas

61 -3) with magnetic fields up to around 10(15) gauss, luminosities of approximately 10(31)-10(36) ergs

62 15 outburst, we present a precise 461 +/- 12 gauss magnetic field measurement in the corona.

63 eeman shift approximately 4 x 10(-18) at 0.1 Gauss magnetic field, compared to approximately 10(-8) f

64 We show that the probability p(t) that a Gauss-Markov process will first exceed the boundary at t

65 Furthermore, we applied generalized Gauss-Markov random field smoothing to maintain consiste

66 the Lagrange multipliers in the proof of the Gauss-Markov theorem are tree-additive.

67 The handshake among ML methods, Fourier, and Gauss may help answer the long-standing enigma of seismo

68 find that field strengths larger than ~10(5) gauss may produce the observed depression, and in one ca

69 l an unexpected mapping to the Lennard-Jones-Gauss model normally studied in the context of computati

70 above 80% for 210 Laguerre-Gauss and Hermite-Gauss modes by using vectorial time reversal over an uns

71 ultant modes are similar to truncated Bessel-Gauss modes that exhibit the ability to self-reconstruct

72 re created by the superpositions of Laguerre-Gauss modes with different orders under orthogonal circu

73 orbital angular momentum possessing Laguerre Gauss modes, are favourable as flying information carrie

74 The Gauss modulus critically influences membrane processes t

75 le-splay (Gauss) modulus difference with the Gauss modulus of the L(o) phase being more negative than

76 n that of the L(d) phase and a saddle-splay (Gauss) modulus difference with the Gauss modulus of the

77 ion to the highest fields available, 600,000 gauss, more than a million times the Earth's magnetic fi

78 ce identified limitations in the widely used Gauss-Newton, BFGS and SR1 Hessian approximation schemes

79 GAUSS offers an integrated toolkit for a range of functi

80 f the white dwarf is strong enough (at 10(6) gauss or more) to channel the accreted matter along fiel

81 The field decays at a rate of ~5 Gauss per second for 2 minutes, as measured within a fla

82 The GAUSS platform can reach an ultra-high reaction temperat

83 Our design of the GAUSS platform offers a powerful way to synthesize a var

84 We demonstrate the versatility of the GAUSS platform with the successful synthesis of single a

85 diyne-assisted ultrafast sparking synthesis (GAUSS) platform for the preparation of metastable nanoma

86 is set by determining the optimal number of Gauss points in each sub-element near the crack tip.

87 on the characteristic of the distribution of Gauss points.

88 The GAUSS R package, complete with its source code, is readi

89 tiny seed fields to a level of about 10(-21) gauss (refs 7, 8).

90 The alternative Gauss-Rice approach lifts the resetting of the voltage a

91 Gauss's law dictates that the net electric field inside

92 in individual spins allows us to demonstrate Gauss's law for emergent effective monopoles in two dime

93 In this approach, both of Gauss's laws and Faraday's law are built in as hard cons

94 d DPPC and DMPC bilayers are approximately 1 Gauss smaller (greater) than in the corresponding disper

95 with extremely high magnetic fields ( 10(14) gauss) that exhibit various X-ray phenomena such as spor

96 surface magnetic fields in excess of 10(14) gauss, the decay of which powers a range of high-energy

97 velocity, power, and scan geometry by using Gauss theorem.

98 easurements from a small aircraft by a novel Gauss' Theorem flux integral approach.

99 c ("target") metric and, as a consequence of Gauss' Theorema Egregium, induces strain.

100 o bending, a key driver of such phenomena is Gauss' Theorema Egregium, which implies that naturally f

101 rae of between 2 x 10(4) gauss and 1 x 10(5) gauss, too low to be detectable by other current methods

102 heory is based on the study of iterations of Gauss-type maps, this suggests a connection between the

103 Notably, GAUSS utilizes an expansive, multi-ethnic reference pane

104 Using GAUSS, we analyzed UK Biobank GWAS summary statistics fo

105 at g=2.012 with hyperfine splitting of 17.5 Gauss, which is consistent with nitrosoheme formation an

106 rface dipolar magnetic field of 4.9 x 10(13) gauss, which is higher than those of the vast majority o