ライフサイエンスコーパス: static magnetic field

1 ringing were related to the strength of the static magnetic field.

2 low relaxation of magnetization in a 3000 Oe static magnetic field.

3 absorption spectroscopy in the presence of a static magnetic field.

4 entation of the bicelles with respect to the static magnetic field.

5 e tunable over a wide frequency range by the static magnetic field.

6 perconductivity, acting in a way opposite to static magnetic fields.

7 ups of the Ile, Leu, and Val residues at two static magnetic fields.

8 fference in spectral density J(0) at the two static magnetic fields.

9 igher-resolution machines with high-strength static magnetic fields.

10 of Xenopus embryos were oriented in strong, static magnetic fields.

11 he pulsing rate in the CPMG sequence, at two static magnetic fields, 11.7 and 14.1 T, and three tempe

12 e we show that transcranial application of a static magnetic field (120-200 mT at 2-3 cm from the mag

13 Both static magnetic fields and convective flow can induce th

14 eristics of these radical pairs at different static magnetic fields and ionic strengths.

15 the bound state observed at 14.1 and 23.5 T static magnetic fields, and the small determined R2bound

16 For geometries in which the capillary and static magnetic field are not parallel, the electrophore

17 determine whether the behavioral effects of static magnetic fields are dependent on field strength,

18 High strength static magnetic fields are known to induce vertigo, beli

19 Static magnetic fields as high as 7.0 T did not have a s

20 generated by nuclear spins that precess in a static magnetic field B0 in the presence of magnetic fie

21 Radiofrequency and static magnetic field calculations are used alongside th

22 Recent experiments have shown that intense static magnetic fields can alter the geometry of the ear

23 However, a demonstration that static magnetic fields can influence human brain activit

24 er pulsed EPR spectroscopy up to the highest static magnetic fields currently available.

25 is observation provides a clear example of a static magnetic-field effect on a fundamental cellular p

26 nsitivity independent of the strength of the static magnetic field, extending the applicability of ma

27 20 years, yielding MR systems with stronger static magnetic fields, faster and stronger gradient mag

28 However, the static magnetic field generated by the cellular telephon

29 es of Paramecium caudatum align with intense static magnetic fields >3 Tesla.

30 generating GigaGauss level, solenoidal quasi-static magnetic fields in under-dense plasma using screw

31 is currently lacking, despite evidence that static magnetic fields interfere with neuronal function

32 amental limits in circumstances in which the static magnetic field is not sufficiently strong to trun

33 The control of quasi-static magnetic fields is of considerable interest in ap

34 The shielding of static or quasi-static magnetic fields is typically accomplished through

35 ed nonferromagnetic aneurysm clips to strong static magnetic fields is unlikely to result in any clin

36 ely applied parallel or perpendicular to the static magnetic field, is a valuable technique for study

37 Here we have employed the effects of weak static magnetic fields (not exceeding 46 mT) on radical

38 d magnetic resonance imaging scanners with a static magnetic field of 3 Tesla or higher are becoming

39 a robust nystagmus while simply lying in the static magnetic field of an MRI machine.

40 The static magnetic field of the MR imaging device affects t

41 otein-containing bicelles are aligned in the static magnetic field of the NMR spectrometer.

42 the transmembrane domain with respect to the static magnetic field, of 21 +/- 2 degrees and, at the s

43 Static magnetic field, or B0, and combined transmit and

44 T) schemes utilize very low frequency, quasi-static, magnetic fields; power transfer occurs via magne

45 H}-15N NOE data collected at 500 and 700 MHz static magnetic fields showed that the internal motions

46 In contrast, the effects of a homogeneous, static magnetic field (SMF) on Central Nervous System (C

47 udy aims to examine the influence of a 0.5 T static magnetic field (SMF) on yeast and human embryonic

48 ng hit by ferromagnetic objects attracted by static magnetic field (SMF) produced by scanner magnet -

49 modulated radiofrequency (PRF) signal, and a static magnetic field (SMF), applied independently, incr

50 We demonstrate that transcranial static magnetic field stimulation (tSMS) over the somato

51 Transcranial static magnetic field stimulation (tSMS) was recently in

52 er a temperature range of 290-320 K and at a static magnetic field strength of 14.1 T.

53 ation is static (continuous, proportional to static magnetic field strength, requiring neither head m

54 elmi coils are compatible with MR imaging at static magnetic field strengths of 1.5 T or less.

55 ame relaxation data acquired at 310 K and at static magnetic field strengths of 11.7, 14.1 and 18.8 T

56 ed electrons in the diffraction peaks with a static magnetic field to obtain the time-dependent diffr

57 lysis of k(CR) in the presence of an applied static magnetic field was used to extract the singlet an

58 Static magnetic fields were not found to have a signific

59 ucture but align differently relative to the static magnetic field when dissolved in a liquid crystal

60 ation within 3D images in a 1D inhomogeneous static magnetic field with a matched rf field gradient.

61 cells exposed during 72 h to a 0.5 T uniform static magnetic field with those of unexposed cells.