ライフサイエンスコーパス: full width at half maximum

1 although there was no significant change in full width at half maximum.

2 ith a beam size of approximately 1.5 degrees full width at half maximum.

3 e entire peak, rather than extrapolating the full-width at half-maximum.

4 to-cathodic peak separations and anodic peak full widths at half-maximum.

5 le dose distribution centered around 103 Gy (full width at half maximum, 20 Gy).

6 chieve effective resolutions of up to 7.5-nm full width at half maximum (3.2-nm localization precisio

7 ned on an intermediate resolution tomograph (full width at half maximum, 8 mm); the subsequent 18 pat

8 Full width at half-maximum analysis (fwhm) was performed

9 objective problem were the ratio between the full width at half-maximum and the half-maximum intensit

10 Peak widths of Deltam/z 0.6 Th (full width at half-maximum) and a mass range of up to m/

11 ructure having the broadest emission (183 nm full width at half-maximum) and longest lifetime (tauavg

12 asmon resonance lineshapes (down to a few nm full-width-at-half-maximum) and the generation of singul

13 signal (lambda(max)(T(1)-->T(n)) = 1150 nm; full width at half-maximum approximately 350 cm(-1)), an

14 ons have a mean energy of 3 MeV per nucleon (full-width at half-maximum approximately 0.5 MeV per nuc

15 ax = 568 nm, etaext = 1.9%) with an emission full width at half-maximum as narrow as 70 nm.

16 urce in the transaxial direction was 4.6 mm (full width at half maximum) at the center, and the axial

17 tor, energy resolution values of 1 keV fwhm (full width at half-maximum) at 5.5 MeV have been achieve

18 The PL line width of HgTe NPLs (40 nm full width at half-maximum, centered at 880 nm) is a fac

19 e obtained have narrow emission spectra with full-width at half-maximum close to 20 nm, and quantum y

20 nchronous mode-locked operation, pulses with full-width at half maximum durations of 610 fs and 1.68

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

22 the HEGP collimator (e.g., 0.9 vs. 1.4 cm in full width at half maximum for (131)I).

23 The spatial resolution was 2.4 mm in full width at half maximum for image planes parallel to

24 transaxial resolution for 2D (3D) was 5.1 mm full width at half maximum (FWHM) (5.0 mm) at 1 cm from

25 The 2D NU94 transaxial resolution is 6.1-mm full width at half maximum (FWHM) 1 cm off center and in

26 backprojection algorithms were below 1.8-mm full width at half maximum (FWHM) at the center of the f

27 A full width at half maximum (FWHM) DOI resolution of 2 mm

28 on at postinjection counting rates was 11.7% full width at half maximum (FWHM) for 662-keV gamma-rays

29 ucibility was found at a filter size of 8-mm full width at half maximum (FWHM) for elasticity and pro

30 profile and depth resolutions approaching a full width at half maximum (fwhm) of 5 nm can be achieve

31 The full width at half maximum (FWHM) of the average in vivo

32 The average full width at half maximum (FWHM) of the SLNs in the pho

33 itude enhancement) and sharp resonances with full width at half maximum (FWHM) of ~15 nm in the zero-

34 Spectral resolution as low as 2.5 nm full width at half maximum (fwhm) was measured using an

35 PET insert device ranges from 1.1- to 1.4-mm full width at half maximum (FWHM) without correction for

36 In terms of sensitivity to full width at half maximum (FWHM), 15 TFs and 1 FOS had

37 0(5) photons in a spectral bandwidth of 50% full width at half maximum (FWHM).

38 he coincidence timing resolution was 1.42-ns full width at half maximum (FWHM).

39 ibration procedure the link between the peak full width at half-maximum (fwhm) and the drift time of

40 ume combustion interface to preserve <300 ms full width at half-maximum (fwhm) fast GC peaks generate

41 eviations of the peak area, peak height, and full width at half-maximum (fwhm) for the internal stand

42 ried out with resolution in excess of 25,000 full width at half-maximum (fwhm), it became possible to

43 MeV) and (241)Am gamma-rays (59.5 keV), with full widths at half-maximum (FWHM, in percentage) of 19%

44 ce ratio (F/F(0)) of approximately 2.0 and a full-width at half maximum (FWHM) of approximately 1 mic

45 omogeneous transitions at 708 nm and 714 nm (full-width at half-maximum (fwhm) approximately 200--300

46 Semi-automatic techniques, using full-width at half-maximum (FWHM) criterion, correlated

47 ocrystals ranged from 20% to 40%, and the PL full-width at half-maximum (fwhm) was maintained between

48 The reconstructed probe shows a full-width-at-half-maximum (FWHM) peak size of 11.2 nm.

49 inal cohort: 22 PD, 20 N; resolution: 7.5 mm full width at half maximum [FWHM]); group B (18 PD, 12 N

50 rdiopulmonary transit times and dispersions (full widths at half maximum [FWHM]) were determined from

51 provides a 1.7-fold increase in resolution (full width at half maximum, fwhm) as well as reduced pea

52 T(n) absorption manifold spectral bandwidth (full width at half-maximum, fwhm, approximately 2000-250

53 The averaged full widths at half maximum (FWHMs) of the radial/tangen

54 spectrum and wide spectral stop-band widths (full-width at half-maximum >80 nm), while preserving the

55 he resolution varied from 1.50 to 2.01 mm in full width at half maximum in the radial direction and f

56 atial resolution ranged from 1.17 to 1.86 mm full width at half maximum in the radial direction from

57 nal stray light (large-angle domain) and the full-width-at-half-maximum intensity of the point-spread

58 Interictal SPECT with 6-8-mm full-width at half-maximum is an alternative to PET.

59 n, R = m/delta m, where delta m, measured as full width at half-maximum, is estimated as 100.

60 (2.7 +/- 0.2 nm) and narrow emission bands (full width at half-maximum <20 nm).

61 ed by visual scoring and quantified with the full-width at half-maximum method.

62 ion of the system ranges from 1.0- to 1.8-mm full width at half maximum near the center of the FOV, d

63 A (12)C beam with a full width at half maximum of 10 mm was delivered to the

64 urin molecules peaks at 45.7+/-0.5 mV with a full width at half maximum of 15 mV vs saturated calomel

65 lung (-850 to -701 HU) greater than 1 L; and full width at half maximum of attenuation-frequency dist

66 o cardiac motion, leading to improvements in full width at half maximum of the canine myocardium of 1

67 e spatial resolution was determined from the full width at half maximum of the detected point spread

68 The shape and measured full width at half maximum of the line spread functions

69 The full width at half maximum of the line-spread function a

70 o assess left ventricle (LV) wall thickness (full width at half maximum of the medial sections), TD,

71 The full width at half maximum of the transverse line spread

72 CBV, with an onset time (OT) of 350 ms and a full width at half-maximum of 1 s.

73 h a decay half-time of 20.8 +/- 0.2 ms and a full width at half-maximum of 1.40 +/- 0.03 microm (mean

74 with amplitudes between 55 and 120 V/cm and full width at half-maximum of 65-100 ms.

75 er centered at 945 cm(-)(1) with a pass-band full width at half-maximum of 93 cm(-)(1).

76 er and follow a Gaussian distribution with a full width at half-maximum of approximately 0.35 mm.

77 The resulting Pdots exhibit the emission full width at half-maximum of approximately 36 nm, which

78 atinum electrodes exhibited redox peaks with full width at half-maximum of approximately 45 mV, much

79 th atomic force microscopy and show that the full width at half-maximum of features approximately 86

80 rom each other in an image, and the apparent full width at half-maximum of small particles.

81 ed through peak shifts and variations of the full width at half-maximum of specific Raman lines, resp

82 as high as 85% at room temperature, and the full width at half-maximum of the corresponding PL peak

83 n tunnelling through CdSe quantum dots, with full widths at half maximum of only ~15 mV at room tempe

84 tion edge, we find a red-shifted, broadband (full-width at half-maximum of about 0.4 eV), emission ba

85 fluorescence domains were estimated from the full-width at half-maximum of gaussian fits to isochrona

86 Full-width at half-maximum of mass spectral peaks was fo

87 The spectral full-width at half-maximum of the emission is reduced fr

88 The spatial resolution, measured as full width at half maximum on single-slice rebinning/fil

89 comprise a well-defined Gaussian peak with a full width at half-maximum ranging from 4 to 30 nm.

90 yzed by using both fixed- and variable-size (full-width-at-half-maximum) ROI measures of the DOS tota

91 accuracy differing by about 20%-50% between full-width-at-half-maximum settings of 5.0 and 7.5 mm.

92 ct border zone mass was 29.8 g (3.9-60.2 g) (full-width at half-maximum, signal intensity thresholdin

93 two or three narrow peaks of 300- to 600-nm full width at half-maximum that maintain their positions

94 tector, the system resolution was 1.5-1.9-cm full width at half maximum, the sensitivity was (0.6-1.5

95 icrovessels were determined by measuring the full width at half maximum through the vessels in the MS

96 p-field experiment and processing the peak's full width at half-maximum to reconstruct CCSDs.

97 The full width at half maximum transverse resolution at a 1-

98 ngated and software-gated images, and lesion full width at half maximum values decreased by 9.9% +/-

99 (221 msec +/- 6); shape was characterized by full width at half maximum values of 174 msec +/- 11, 98

100 kPa was generated with modulated peak fwhm (full width at half-maximum) values ranging from 90 to 64

101 We demonstrate the first sub-100 nm full-width-at-half-maximum visible-blind red and NIR pho

102 lope became steeper by 66.7% (P = 0.001) and full width at half maximum was reduced by 20.6% (P = 0.0

103 he estimated cerebral blood flow response at full width at half-maximum was 470 microm under single-s

104 orobenzene is shown to be approximately 180 (full width at half-maximum), with no significant loss in