ライフサイエンスコーパス: FWHM

1 FWHM averaged differences of - 0.20, - 0.28, and - 0.15

2 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

3 ximum (FWHM) and an energy resolution of 13% FWHM were obtained in the uniform glass light-guide modu

4 4.3 mum and an absorption bandwidth of 170% FWHM on 15.8 mum center wavelength, coincident with impo

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

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

7 pollution and constant signals (%RSD = 8.5%, FWHM of 177 ms +/- 8.5%, n = 10 557).

8 f 2.5 mm FWHM and an energy resolution of 9% FWHM.

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

10 uction smoothing, Abeta- CLs increased for a FWHM of 4.5 mm or more, whereas Abeta+ CLs decreased acr

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

12 highest dose rates obtained for beams with a FWHM of about 2 cm and +/- 10% uniformity over 1 cm diam

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

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

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

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

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

18 ct on the features than iteration number and FWHM.

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

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

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

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

23 m found for the viral mobility distribution (FWHM(Z) < 3.7%) is substantially narrower than that repo

24 peak pressures of ~ 1 MPa and spatial extent FWHM ~ 36 um.

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

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

27 ly in low conductance regime and increase in FWHM of focusing peak is observed.

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

29 - 0.6), spatial width at half-max intensity (FWHM = 2.7 +/- 1.2 vs. 2.6 +/- 0.6 microm), nor the dura

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

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

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

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

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

35 Subsequently, full width half max (FWHM) of the stenosis, Dice score (DSC) for the stenosed

36 (3D) was 5.1 mm full width at half maximum (FWHM) (5.0 mm) at 1 cm from gantry center and the radial

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

38 lution of 5.0 mm full width at half maximum (FWHM) and an energy resolution of 13% FWHM were obtained

39 nm with a narrow full-width at half maximum (FWHM) at 44 nm and a quantum yield of 15.5%.

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

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

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

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

44 ion (SD) and the full width at half maximum (FWHM) methods.

45 response with a full width at half maximum (FWHM) of <50 nm, and tunability to cover the NIR-I range

46 of 569 nm with a full width at half maximum (FWHM) of 208 nm.

47 PLQY and narrow full width at half maximum (FWHM) of 75 meV (30 nm).

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

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

50 The intensity and full width half maximum (FWHM) of the focusing peak are associated with the colli

51 Full width at half maximum (FWHM) of the resonance modes increased with increasing t

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

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

54 as calculated as full width at half maximum (FWHM) using the barrel phantom method.

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

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

57 rrow linewidths (full width at half maximum (FWHM) ~ 62-64 km s(-1)).

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

59 5.0% to 69.6% in full width at half maximum (FWHM), with a mean of 19.3% +/- 3.7%.

60 bandwidth of 50% full width at half maximum (FWHM).

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

62 ips with angular full-width-at-half-maximum (FWHM) < 1.5 degrees , resulting in an order-of-magnitude

63 peaks with 0.45 nm Full-Width-Half-Maximum (FWHM) can be clearly resolved.

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

65 th relative full peak width at half-maximum (FWHM) in mobility approaching 2% (~1% in diameter).

66 tions in 63 s at full width at half-maximum (FWHM) of 105 ms and a relative standard deviation (%RSD)

67 at 617 nm with a full width at half-maximum (FWHM) of 284 nm (0.96 eV).

68 hotoluminescence full-width at half-maximum (FWHM) of about 120 meV throughout.

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

70 (SPP), achieving full-width at half-maximum (FWHM) values below 2 s (Zoom 120) and 3 s (Zoom 80).

71 59.5 keV), with full widths at half-maximum (FWHM, in percentage) of 19% and 50%, respectively.

72 ead of ~ 3.2 um (full width at half maximum [FWHM]) and are observed with a mean spatial frequency of

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

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

75 a(PL) of 410 nm, full width at half maximum, FWHM, of 38 nm, photoluminescence quantum yield, Phi(PL)

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

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

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

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

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

81 oint source in air averaged 0.81 +/- 0.11 mm FWHM.

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

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

84 nsic spatial resolution was 1.30 and 1.38 mm FWHM in the transverse and axial directions, respectivel

85 T module achieved a DOI resolution of 2.5 mm FWHM and an energy resolution of 9% FWHM.

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

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

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

89 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

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

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

92 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.

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

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

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

96 e-particle localization precision of 100 nm (FWHM) and <10 nm (1o), respectively.

97 ectroluminescence spectrum peaked at 409 nm (FWHM=37 nm) and a maximum external quantum efficiency (E

98 nd BN-Se show narrowband emission at 483 nm (FWHM of 22 nm) and 485 nm (FWHM of 22 nm).

99 ission at 483 nm (FWHM of 22 nm) and 485 nm (FWHM of 22 nm).

100 This exceptional value of FWHM is attributed to the remarkable uniformity in both

101 ickness and E contributed to the variance of FWHM.

102 effect of heart rate and acquisition mode on FWHM at diastole (p-values < 0.001).

103 -quality MALDI MS images at resolving power (FWHM) above 1,000,000 in the lipid mass range across the

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

105 age coincidence time resolution was 375.4 ps FWHM.

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

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

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

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

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

111 20, - 0.28, and - 0.15 mm relative to static FWHM at VMI 150 keV across acquisition parameters for hi

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

113 The FWHM of Pb,Br,H,Cs,Na-X, however, is narrower than any p

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

115 ore, whereas Abeta+ CLs decreased across the FWHM range.

116 - and the Abeta+ groups were impacted by the FWHM of the reconstruction method.

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

118 sible protein-dye interactions increased the FWHM slightly.

119 either time-domain transient signals or the FWHM of frequency domain peaks in FT mass analyzers.

120 4 microm, approximately 82% greater than the FWHM of the diffraction-limited LSF.

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

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

123 tly found for several non-enveloped viruses (FWHM(Z) 2%), presumably due to particle to particle vari

124 in CLs between Abeta- and Abeta+ groups with FWHM were examined.

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

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

127 0 pA simultaneously, can produce sparks with FWHM approximately 2 microm.