ライフサイエンスコーパス: gauss

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

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

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

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

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

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

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

8 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

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

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

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

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

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

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

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

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

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

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

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

20 Gauss et al. present evidence that an endoplasmic reticu

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

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

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

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

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

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

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

28 15 outburst, we present a precise 461 +/- 12 gauss magnetic field measurement in the corona.

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

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

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

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

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

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

35 The Gauss modulus critically influences membrane processes t

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

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

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

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

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

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

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

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

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

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

46 tasets and R package are available at http://gauss.usouthal.edu/publ/beadsme/.

47 tasets and R package are available at http://gauss.usouthal.edu/publ/logit/.

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

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