ライフサイエンスコーパス: FWHM

1 cells) the amplitude was 1.30 (0.84, 2.08), FWHM was 1.63 (1.02, 2.66) microm, and FDHM was 43.6 (23

2 s (n = 284 sparks), DeltaF/Fo = 1.9 +/- 0.4, FWHM = 5.1 +/- 1.5 micrometer, and Deltat = 168 +/- 43 m

3 verage photopeak energy resolution was 9.40% FWHM, and the average coincidence time resolution was 37

4 ual Ca2+ sparks with peak F/F(0) of >6 and a FWHM of approximately 2 microm, and a mathematical model

5 s that small-animal PET systems capable of a FWHM spatial resolution of 600 microm or less are feasib

6 maximum (FWHM) DOI resolution of 2 mm and an FWHM energy resolution of 15% were obtained at a tempera

7 pes, the frequency of sparks, DeltaF/Fo, and FWHM were gradually decreased by tetracaine and increase

8 ulting in a better Q value than with MAX and FWHM for all noise, background and spatial resolutions.

9 ed more linearly with thickness than MAX and FWHM, resulting in a better Q value than with MAX and FW

10 Iteration number and FWHM of the gaussian filter have a similar impact on the

11 ct on the features than iteration number and FWHM.

12 Transit times and FWHM values for the patients with heart failure were com

13 Cardiopulmonary transit times and FWHM values were significantly prolonged in the patients

14 NU01 2D average transaxial (axial) FWHM resolution measured 6.1 (5.2) mm at R = 1 cm and 6.

15 cross this spectral window produces a broad (FWHM approximately 60 nm) but clearly resolved feature c

16 spatial width at half-maximal fluorescence (FWHM) was 3.6 +/- 1.1 micrometer and the full duration o

17 HYB, 95% and 50% for MAX and 100% and 0% for FWHM, respectively).

18 unt-based index (MAX) and a geometric index (FWHM).

19 - 0.6), spatial width at half-max intensity (FWHM = 2.7 +/- 1.2 vs. 2.6 +/- 0.6 microm), nor the dura

20 o) vs. full width at half-maximal intensity (FWHM) vs. full duration at half-maximal intensity (FTHM)

21 CE MR-derived PTT, LV FWHM, and LV TTP are noninvasive compound markers of pul

22 PTT, LV FWHM, and LV TTP correlated with pulmonary vascular resi

23 tricles, and right-to-left-ventricle PTT, LV FWHM, and LV TTP were calculated.

24 orescence, the full width at half-magnitude (FWHM) was 1.4 (0.9, 2.3) microm, and the full duration a

25 (3D) was 5.1 mm full width at half maximum (FWHM) (5.0 mm) at 1 cm from gantry center and the radial

26 lution is 6.1-mm full width at half maximum (FWHM) 1 cm off center and increases to 6.9 mm tangential

27 ere below 1.8-mm full width at half maximum (FWHM) at the center of the field of view.

28 A full width at half maximum (FWHM) DOI resolution of 2 mm and an FWHM energy resoluti

29 rates was 11.7% full width at half maximum (FWHM) for 662-keV gamma-rays.

30 ter size of 8-mm full width at half maximum (FWHM) for elasticity and propagation parameter beta and

31 mately 2.0 and a full-width at half maximum (FWHM) of approximately 1 microm.

32 The full width at half maximum (FWHM) of the average in vivo line-spread function (LSF)

33 The average full width at half maximum (FWHM) of the SLNs in the photoacoustic images at three i

34 resonances with full width at half maximum (FWHM) of ~15 nm in the zero-order transmission using an

35 minescence emission full width half maximum (FWHM) values below 40 meV and emission intensities nearl

36 m 1.1- to 1.4-mm full width at half maximum (FWHM) without correction for the point-source dimension.

37 f sensitivity to full width at half maximum (FWHM), 15 TFs and 1 FOS had the best performance with a

38 andwidth of 50% full width at half maximum (FWHM).

39 tion was 1.42-ns full width at half maximum (FWHM).

40 echniques, using full-width at half-maximum (FWHM) criterion, correlated best with postmortem data (r

41 ed probe shows a full-width-at-half-maximum (FWHM) peak size of 11.2 nm.

42 59.5 keV), with full widths at half-maximum (FWHM, in percentage) of 19% and 50%, respectively.

43 nd dispersions (full widths at half maximum [FWHM]) were determined from the curves.

44 solution: 7.5 mm full width at half maximum [FWHM]); group B (18 PD, 12 N; resolution: 4.2 mm FWHM);

45 Ca2+ sparks are consistent with the measured FWHM of approximately 2 microm, and that the underlying

46 M); group C (25 PD, 15 N; resolution: 8.0 mm FWHM); and group D (14 PD, 10 N; resolution: 10 mm FWHM)

47 t the center of the field of view was 1.0-mm FWHM with 20 DOI bins and was not measurable when using

48 and group D (14 PD, 10 N; resolution: 10 mm FWHM).

49 t in spatial resolution (from 17 mm to 11 mm FWHM) as well as contrast resolution (from 34% to 45%),

50 and propagation parameter beta and at 16-mm FWHM for viscosity and attenuation parameter alpha.

51 ]); group B (18 PD, 12 N; resolution: 4.2 mm FWHM); group C (25 PD, 15 N; resolution: 8.0 mm FWHM); a

52 d the axial resolution remained under 2.5-mm FWHM within the central 4-cm diameter of the field of vi

53 was 0.9-mm FWHM with 20 DOI bins and 1.6-mm FWHM with 1 DOI bin.

54 The intrinsic spatial resolution was 0.68-mm FWHM as measured with a 30-gauge needle filled with (18)

55 The axial resolution for 2D (3D) was 4.8 mm FWHM (5.8 mm) and 6.3 mm (6.5 mm) at 1 cm and 10 cm from

56 tion of the original scanner (1.7- to 1.8-mm FWHM) in 2 of the 3 directions.

57 e viscoelasticity up to a resolution of 8-mm FWHM.

58 t the center of the field of view was 0.9-mm FWHM with 20 DOI bins and 1.6-mm FWHM with 1 DOI bin.

59 Intrinsic spatial resolution was 2.7 mm (FWHM) at 662 keV.

60 oduced up to several hundred narrow (< 20 ms FWHM [full width at half maximum]) fluorescence peaks.

61 photon numbers of an ultrabroadband (110 nm FWHM) squeezed state in the telecom band centred at 1535

62 eved with the Discovery MI, including 375 ps FWHM coincidence time resolution and sensitivity of 14 c

63 age coincidence time resolution was 375.4 ps FWHM.

64 In multiple linear regression models, PTT, FWHM, and TTP were associated with mean pulmonary arteri

65 ed; the best spectrometer energy resolution (FWHM) achieved at 5.9 keV was 900 eV for the 200 mum In0

66 ator surface, the planar spatial resolutions FWHM in mm (point source sensitivities in cps-MBq) for h

67 SPECT resolutions (FWHM) at the center of rotation were 8.1-11.9 mm (lead)

68 nds; 25th-75th percentile, 6.9-9.9 seconds), FWHM (median, 8.2 seconds; 25th-75th percentile, 5.7-11.

69 that also enforces a local biaxial texture (FWHM <15 degrees ) while simultaneously allowing the c-a

70 (n = 426 sparks), DeltaF/Fo = 1 +/- 0.5, the FWHM = 2.5 +/- 1.1 micrometer, and Deltat = 97 +/- 50 ms

71 However, the FWHM of the SLNs in fluorescence images widened from 8 t

72 sible protein-dye interactions increased the FWHM slightly.

73 4 microm, approximately 82% greater than the FWHM of the diffraction-limited LSF.

74 By contrast Bi2223 shows only a uniaxial (FWHM <15 degrees ) c-axis texture perpendicular to the t

75 Using FWHM, there was no difference in MI size between differe

76 y 11 pA needed to generate a Ca2+ spark with FWHM of 2 microm.

77 veral factors that might produce sparks with FWHM approximately 2 microm without using large currents

78 0 pA simultaneously, can produce sparks with FWHM approximately 2 microm.