ライフサイエンスコーパス: cm

1 uptake, and only a third of metastases < 1.0 cm were (18)F-FET-negative, most likely because of scann

2 lows southwestward with core velocity of 2.0 cm/s and a volume transport of 1.65 Sv (1 Sv = 1 x 10(6)

3 city = 9.3+/-2.4 cm/second versus 11.1+/-2.0 cm/second; P<0.001).

4 (airway pressures of 14/0, 30/0, 45/10, 45/0 cm H2O).

5 n LV end-diastolic diameters (5.2 versus 6.0 cm; P=0.001), greater relative wall thickness (0.41 vers

6 An ultrahigh Hall mobility value of >20,000 cm(2) V(-1) s(-1) is measured in as-grown Bi2O2Se nanofl

7 contains an ultra-high density array (10,000/cm(2)) of short ( 230 mum) microprojections that deliver

8 the reduced mobility values of 1.99 +/- 0.01 cm(2) V(-1)s(-1) at 175 degrees C.

9 moderate certainty evidence) or height (0.07 cm, 95% CrI -0.10 to 0.24; moderate certainty evidence),

10 iencies (PCEs) of small-area devices (</=0.1 cm(2) ), the PCEs deteriorate drastically for PSCs of la

11 a and penetrating the seabed on average 16.1 cm.

12 hest average field-effect hole mobility (5.1 cm(2) V(-1) s(-1)).

13 iled chambers (oil thickness approximately 1 cm) compared to unoiled chambers, as the majority ( appr

14 t with high-yield (>98%) over large areas (1 cm(2)) and of general validity for both conjugated and n

15 Speeds ranged from 1 cm/sec to 4.5 cm/sec.

16 regular Z line and patients with BE of >/= 1 cm did not differ significantly in age, race, or duratio

17 or EAC developed in patients with BE of >/=1 cm in length.

18 reasonable and that if cytoreduction to < 1 cm of residual disease seems feasible, to proceed with P

19 BACKGROUND & AIMS: Many patients with a < 1 cm segment of columnar metaplasia in the distal esophagu

20 crystals to grow to lateral dimensions of 1 cm ( 30,000 of unit cells) and thickness of 100 mum (

21 conditions (25 degrees C, air flow rate of 1 cm(3) min(-1)).

22 arized and detected in locations more than 1 cm apart.

23 (-1)) and 1.0(3) x 10(-3) S/cm (Ea = 0.19(1) cm(-1)) in its solvated and desolvated forms, respective

24 o sigma = 1.4(7) x 10(-2) S/cm (Ea = 0.26(1) cm(-1)) and 1.0(3) x 10(-3) S/cm (Ea = 0.19(1) cm(-1)) i

25 n the novel lightweight steel (227 MPa g(-1) cm(3) ).

26 f the macrofiber is as high as 598 MPa g(-1) cm(3) , which is even substantially stronger than the no

27 Cotton effects (Deltaepsilon = +/-100 M(-1) cm(-1) at 300 nm).

28 extinction coefficient of 1.90 x 10(5) m(-1) cm(-1) in solution.

29 ity increase of up to epsilon = 120000 M(-1) cm(-1).

30 sensitivities were 21.8 and 14.4 muA muM(-1) cm(-2), with detection limits of 18.1 +/- 1.22 and 1.38

31 of the biosensor for CC is 0.932 muMmuA(-1) cm(-2), 2 s and 0.085 muM, respectively.

32 M with a sensitivity of 0.172microAmicroM(-1)cm(-2).

33 oved superoxide sensitivity of 7.29nAnM(-)(1)cm(-)(2) and a low level of detection of 70pM.

34 or exhibited high sensitivity (15.31muAmM(-1)cm(-2)) for the detection of glucose over a concentratio

35 tinction coefficient 23.2 (+/-0.3)x10(3)M(-1)cm(-1)).

36 6.5 mM with a sensitivity of 191.6 muA mM(-1)cm(-2) and a detection limit of 1.1 x 10(-3) mM.

37 e mother and 1% to 2% for each additional 10 cm of height.

38 revious experimental observations (k(0) > 10 cm/s).

39 ht (reference was the taller sibling): >/=10 cm difference between brothers hazard ratios=0.69 (95% c

40 ight was calculated on tomography, and >/=10 cm(2)/m was considered abnormal, as previously reported.

41 1 reticular vein with a minimum length of 10 cm in 1 of their lower limbs.

42 An increase of 10 cm in genetically determined height was associated with

43 abrication protocol for laboratory scale (10 cm(2)) fuel cells based on ultrasonic spray deposition o

44 h specificity by using a PSV greater than 10 cm/sec and an RI greater than 0.65 as diagnostic criteri

45 to reveal a bipolaron sheet density >10(10) cm(-2) at the interface between an indium tin oxide anod

46 loss compared to the bandgap and high (>100 cm(2) V(-1) s(-1) ) intrinsic carrier mobilities.

47 l vascular network encompassing an area >100 cm(2) We found that the collagen cross-linking enzyme ly

48 ally obese men (waist circumference: 102-110 cm) participated.

49 on of a pore volume variation from 10 to 110 cm(3)/g by cobalt insertion in the MoS2 crystallographic

50 lity for Hg3Se2I2 is estimated as 104 +/- 12 cm(2)/(V.s).

51 a specific detectivity value of 1.2 x 10(12) cm.Hz(1/2)/W.

52 with a record anisotropy barrier up to 1277 cm(-1) (1837 K) in zero field and a record magnetic bloc

53 nd sheet carrier density above 1.07 x 10(13) cm(-2) .

54 decreased from 165 (126-179) to 72 (54-137) cm H2O * s/min, respectively (p = 0.033).

55 low trap density ( approximately 4 x 10(14) cm(-3) ), and unprecedented 9 GHz charge-carrier mobilit

56 obe 15 cm up to the MIRUS system (S1) and 15 cm from the filter-Reflector group (S2).

57 gth for Raman gas sensing was found to be 15 cm in our spectroscopic system.

58 eline) and during sedation with the probe 15 cm up to the MIRUS system (S1) and 15 cm from the filter

59 or effective diameter ranges of less than 15 cm, 15-19 cm, 20-24 cm, 25-29 cm, and greater than or eq

60 Specifically, a 1545 cm(-1) band increased in intensity with the progression

61 f a computed tomography (CT) scanner with 16-cm coverage and 230-microm spatial resolution at coronar

62 TFA absorbs as a strong sharp peak (1675 cm(-1)) within the amide I' band of the spectral region.

63 ve diameter ranges of less than 15 cm, 15-19 cm, 20-24 cm, 25-29 cm, and greater than or equal to 30

64 of age), sex, or height (among donors </=190 cm tall).

65 th regard to age, sex, and height (if </=190 cm).

66 level of 62.5 mol % cholesterol and 10 +/- 2 cm/s in a 100% cholesterol mimic of the experimentally o

67 senteric artery (SMA) with a diameter of 2.2 cm was found incidentally on an ultrasound (US) examinat

68 lly appropriate cutoffs for tumor size (<2.2 cm, >/=4.8 cm,) and nodal status (no positive nodes, 1 t

69 reases from the original value of 1.8 to 3.2 cm(2) V(-1) s(-1) .

70 5.5 kg/m(2); mean length of BE, 3.7 +/- 3.2 cm).

71 bility decreases somewhat, reaching 40 +/- 2 cm/s at the near-saturating level of 62.5 mol % choleste

72 ation, 6 cm H2O above; open lung approach, 2 cm H2O above; and collapse, 6 cm H2O below the highest c

73 nd-expiratory pressure titration (steps of 2 cm H2O starting from >/= 26 cm H2O).

74 ot ultralow risk," tumor size greater than 2 cm was the most predictive of outcome.

75 gh mobility-lifetime product of 1.8 x 10(-2) cm(2) V(-1).

76 Samples collected near the surface (0-20 cm) and deeper (20-40 cm) both increased by an average o

77 ith filtered backprojection at 1, 10, and 20 cm from the system center were, respectively, 4.10/4.19/

78 The 10 to 20 cm of sea-level rise expected no later than 2050 will mo

79 reatments with fine sediment in the upper 20 cm of the columns showed high phosphorus retention.

80 mance, with electron mobility exceeding 2000 cm(2) V(-1) s(-1) and sheet carrier density above 1.07 x

81 V positron beam with density of 2.5 x 10(22) cm(-3) and flux of 1.6 x 10(10)/shot is achieved.

82 e hole carrier density (varying from >10(22) cm(-3) to intrinsic) in copper sulfide nanocrystals by e

83 r ranges of less than 15 cm, 15-19 cm, 20-24 cm, 25-29 cm, and greater than or equal to 30 cm, respec

84 ater level fell below a tipping point of -24 cm.

85 , those living at least 2000 m away had 0.26 cm smaller waist circumference (-0.52 to 0.01).

86 tion (steps of 2 cm H2O starting from >/= 26 cm H2O).

87 positive airway pressure of 24 (IQR, 22-26) cm H2O, an expiratory positive airway pressure of 4 (IQR

88 -kg lower body weight (P < 0.001) and a 0.26-cm(3) lower AFA (P < 0.01).

89 f less than 15 cm, 15-19 cm, 20-24 cm, 25-29 cm, and greater than or equal to 30 cm, respectively.

90 ntracta width (1.1+/-0.5 cm versus 0.6+/-0.3 cm; P=0.001), and regurgitant volume (57.2+/-12.8 mL/bea

91 , 41% were women, mean lesion length was 8.3 cm, and 44% were severely calcified.

92 4:00, the largest measuring approximately 3 cm on exam, and multiple palpable right axillary lymph n

93 AFP > 200 (P < 0.0001, HR: 3.8), and Size >3 cm (P < 0.001, HR: 3.2).

94 cinoma of grade 1-3, with a tumour size of 3 cm or less (pT1-2), none to three positive axillary node

95 s for longer than 3 weeks, thrombus within 3 cm of the sapheno-femoral junction, indication for full-

96 effects of treatment extend passively 20-30 cm below the depth of the original amendment.

97 etermined on an equivalent mass basis to 30 cm soil depth.

98 m, 25-29 cm, and greater than or equal to 30 cm, respectively.

99 fferent working distances (far, 60 cm and 33 cm) and impact on vision quality of multifocal IOLs Acry

100 far (4 m), intermediate (60 cm) and near (33 cm) distances and binocular contrast sensitivity.

101 increasing the density of the beads to 1.3g/cm(3) and the compressive modulus by two orders of magni

102 F parameters: electric field strength of 3kV/cm and pulse width of 10mus after the treatment of 20-h

103 improves the characterization of small (1-4 cm) renal lesions compared with conventional attenuation

104 9 times higher odds of short stature (<155.4 cm), and those born moderately preterm had 1.43 times hi

105 transpulmonary pressure decreased below 2-4 cm H2O.

106 01-0.2%), with large effects on height (>2.4 cm), weight (>5 kg), and body mass index (BMI) (>3.5 kg/

107 enetrating the seabed on average down to 2.4 cm, whereas hydraulic dredges caused the most depletion,

108 ction (early relaxation velocity = 9.3+/-2.4 cm/second versus 11.1+/-2.0 cm/second; P<0.001).

109 exhibiting hole mobility up to 0.15 and 6.4 cm(2) V(-1) s(-1), respectively.

110 cent electrical characteristics (muFE > 64.4 cm(2)/Vs, on/off ratio > 10(6)), and the integrated F-P

111 predominantly in the apical approximately 4 cm of the stem.

112 for inter-electrode distances smaller than 4 cm.

113 cule analysis to be (1.73 +/- 0.08) x 10(-4) cm.s(-1) and 15.71 +/- 0.76 s(-1), respectively.

114 near the surface (0-20 cm) and deeper (20-40 cm) both increased by an average of 9.4 and 5.1 Mg C ha(

115 nental Crust) reveal maximum values 10 to 40 cm below the surface which shows that the zenith of atmo

116 exhibit high Hall mobility values (up to 450 cm(2) V(-1) s(-1)), large current on/off ratios (>10(6))

117 9, standard estimate of error (SEE) = 24.470 cm(2), p < 0.001), Lin's correlation coefficient (CCC) w

118 5 cm of water pressure was delivered via CPAP nasal prongs

119 ing the water-sediment interface and top 0.5 cm of sediments (66%).

120 ); P<0.001), vena contracta width (1.1+/-0.5 cm versus 0.6+/-0.3 cm; P=0.001), and regurgitant volume

121 stics were not found deeper than 3.5 +/- 0.5 cm.

122 hundred and eight patients had cysts </=1.5 cm for more than 5 years of follow-up; only 1 of these p

123 create devices having an active-area of 1.5 cm(2) having an independently verified efficiency of 6.6

124 pair for large segmental radius defects (1.5 cm) in a rabbit model was evaluated by radiography and h

125 rast, among the 255 patients with cysts >1.5 cm, 19 (7.5%) developed malignancy (P = .01).

126 x such that the single cutoff (<11.5 or 12.5 cm) for field screening of acute malnutrition did not tr

127 ible freezing transitions were marked by 2-5 cm(-1) shifts in the radial breathing mode frequency, re

128 tics were found to reside shallower than 2.5 cm sediment depth, with the area of highest microplastic

129 ained 7 irrigated electrodes spaced over 3.5 cm and could deliver </=25 W to each electrode.

130 ductal carcinoma in situ (largest focus, 3.5 cm).

131 Speeds ranged from 1 cm/sec to 4.5 cm/sec.

132 bundance, especially in the fen habitat at 5 cm depth.

133 proved locally advanced pancreatic cancer 5 cm or smaller (13 women, 12 men; median age, 61 years; a

134 on criteria were palpable splenomegaly (>/=5 cm below the left costal margin), Eastern Cooperative On

135 or worse, with palpable spleen of at least 5 cm and without grade 2 or greater peripheral neuropathy

136 10 above positive end-expiratory pressure 5 cm H2O, as well as 5 and 60 minutes postextubation.

137 nd their amplitude increased steeply up to 5 cm inter-electrode distance.

138 ory positive airway pressure of 4 (IQR, 4-5) cm H2O, and a backup rate of 14 (IQR, 14-16) breaths/min

139 trodes with BQ showed 260, 330 and 500microW/cm(2), respectively.

140 ectrodes without BQ were 41, 47 and 53microW/cm(2), while CA, EC and EPC electrodes with BQ showed 26

141 a mean decline in linear extension of -29.56 cm yr(-1) (+/-7.08 SE), which accounted for both erosion

142 ying also increases the hole mobility to 560 cm(2) V(-1) s(-1), yielding a high mobility-lifetime pro

143 strated the greatest shift in mobility (1.58 cm(2)V(-1)s(-1)) compared the DMMP monomer (1.63 cm(2)V(

144 he filter media was recovered in the top 0-6 cm.

145 ve orifice area (from 1.0+/-0.4 to 1.8+/-0.6 cm(2), P<0.001).

146 e was smaller (34.0 +/- 1.5 and 34.3 +/- 1.6 cm, respectively; P = 0.02).

147 s provide exciton diffusion constants of 3-6 cm(2) s(-1) for the tubular molecular aggregates, which

148 thin films on large-format ( approximately 6 cm(2)) single-crystal substrates, and confirm epitaxial

149 ng approach, 2 cm H2O above; and collapse, 6 cm H2O below the highest compliance level.

150 growth (>10 mm/y), aneurysm formation (>/=6 cm), organ or limb ischemia, or new uncontrollable hyper

151 applied in a random order: hyperinflation, 6 cm H2O above; open lung approach, 2 cm H2O above; and co

152 in comparison to the value of 2.38 x 10(-6) cm(2)/s using a standard electrochemical cell.

153 ave a diffusion coefficient of 1.59 x 10(-6) cm(2)/s, in comparison to the value of 2.38 x 10(-6) cm(

154 mes for different working distances (far, 60 cm and 33 cm) and impact on vision quality of multifocal

155 conditions, for far (4 m), intermediate (60 cm) and near (33 cm) distances and binocular contrast se

156 les are taken at a soil depth of at least 60 cm.

157 )V(-1)s(-1)) compared the DMMP monomer (1.63 cm(2)V(-1)s(-1)).

158 ities ranging from approximately 0.03 to 1.7 cm(2) V(-1) s(-1) .

159 mer snowmelt rate increases of up to 6.3% (7 cm a(-1)) on glaciers in three different mountain enviro

160 d with a proxy for solar activity, the F10.7 cm radio flux, and therefore with the solar cycle phase.

161 d MPs with McGowan volumes greater than 1.7 (cm(3) mol(-1))/100.

162 rsus 19 [15-26] and 21 [2-49] versus 4 [0-7] cm(2); P=0.049 and P=0.004, respectively).

163 and extending from 2,300 to well below 1,700 cm(-1) The first contribution corresponds to deprotonati

164 recedented 9 GHz charge-carrier mobility (71 cm(2) V(-1) s(-1) ), is demonstrated.

165 f displaced water libration bands at ca. 730 cm(-1) upon solvent replacement by adsorbed MOP.

166 e coming from landfills in wet climates (>75 cm/yr precipitation) that contain 47% of U.S. solid wast

167 eveals a diatomic Co-O vibration band at 770 cm(-1), which provides the conclusive evidence for the p

168 re PAS was defined as aortic valve area <0.8 cm(2), mean aortic valve gradient >/=40 mm Hg, and dimen

169 iate cutoffs for tumor size (<2.2 cm, >/=4.8 cm,) and nodal status (no positive nodes, 1 to 3 positiv

170 y low methanol permeability of 1.25 x 10(-8) cm(2) s(-1) due to the small pore entrance of the DNA@ZI

171 field effect mobilities (41 for holes and 80 cm(2) V(-1) s(-1) for electrons) and device stability ar

172 rogression involving a soft mode at about 85 cm(-1) These results are rationalized in a vibrationally

173 he protein G-coupled membrane was 43.8microg/cm(2) and the binding efficiency was 88%.

174 n of rotor domains (ablation line, 3.5+/-0.9 cm) effectively decreased the frequency of activation in

175 normal-weight men (waist circumference: <94 cm) and 54 abdominally obese men (waist circumference: 1

176 ard deviation) ranged from -43.950 to 67.951 cm(2), LOA% (given as a percentage of mean value measure

177 (-2) at a constant current density of 0.15 A cm(-2) with a carbon utilization over 85.5%.

178 driving current in the Pt layer from 10(8) A/cm(2) to 10(9) A/cm(2).

179 n the Pt layer from 10(8) A/cm(2) to 10(9) A/cm(2).

180 ed levels at atheroprotective-SS of 12 dynes/cm(2), whereas ICAM-1 rose to a maximum in parallel with

181 nt over a 20mm field ranging from 0-16 dynes/cm(2).

182 VCAM-1 peaked at 2 dynes/cm(2) and decreased to below static TNFalpha-stimulated

183 sors were compared to total fluorine (nmol F/cm(2)) determined by particle-induced gamma ray emission

184 t circumference >94 (males) or >80 (females) cm, serum creatinine <1.2 mg/dL, and normoalbuminuria we

185 ile the density is merely 0.0058 or 0.0089 g cm(-3) , respectively, which far surpasses the best valu

186 cP for viscosity range 0.5-3 cP and 0.0012 g/cm(3) for density range 0.9-1.1 g/cm(3)).

187 loss were -0.02 +/- 0.05 and 0.0 +/- 0.03 g/cm(2) for groups with baseline body mass index (BMI; in

188 0.04 +/- 0.04 compared with -0.02 +/- 0.04 g/cm(2); P = 0.033).

189 d 0.0012 g/cm(3) for density range 0.9-1.1 g/cm(3)).

190 An increase in stress above 2 g/cm(2) did not enhance osteoblastic differentiation furth

191 clastic differentiation were enhanced at 2 g/cm(2).

192 ensity of the mitochondrion was about 1.36 g/cm(3).

193 These compounds possess a high density (>7 g/cm(3)) and wide bandgaps (>1.9 eV), showing great stoppi

194 33 [19-55] Gy cm(2) in 2009 to 27 [16-44] Gy cm(2) in 2013 for CA (P<0.0001), and from 73 [41-125] to

195 rea product was observed, from 33 [19-55] Gy cm(2) in 2009 to 27 [16-44] Gy cm(2) in 2013 for CA (P<0

196 0001), and from 73 [41-125] to 55 [31-91] Gy cm(2) for PCI (P<0.0001).

197 in (p < 0.0001) and 65 Gy.cm(2) versus 59 Gy.cm(2) (p = 0.0001), respectively.

198 : 10 min versus 9 min (p < 0.0001) and 65 Gy.cm(2) versus 59 Gy.cm(2) (p = 0.0001), respectively.

199 e irradiation with heavy ions at 10(16) ions/cm(2) converts WSe2 into a mixture of WOx and Se-deficie

200 h display high-energy densities (up to 166 J cm(-3)) and efficiencies (up to 96%).

201 elivering high energy densities, i.e., 1.2 J cm(-3) , even at a temperature close to the glass transi

202 ial capability under a low light dose (0.6 J cm(-2) ) toward Gram-negative bacteria E. coli, making i

203 VB irradiation and healing (UVB doses 1.01 J/cm(2) once daily for four days).

204 (metal tip) or Er:YAG laser (20.3 or 38.2 J/cm(2)) in non-contact mode.

205 wed low phototoxicity (IC50 > 100 muM, 1.5 J/cm(2)) toward human HEp2 cells.

206 higher electric field ( approximately 10 kV/cm), resulting in various technical difficulties.

207 ation was achieved by bursts of 300-ns, 9 kV/cm pulses (50 Hz, n = 3-100) and quantified by propidium

208 tremely low thresholds on the order of 10 kW cm(-2) at room temperature, which are comparable to thos

209 -circuit current density (J sc ) of 17.07 mA cm(-2) .

210 ectrodes exhibited current densities of 1 mA cm(-2) at 1.07 V vs NHE.

211 hort-circuit current densities up to 42.1 mA cm(-2).

212 ectrocatalytic current density of j = -10 mA cm(-2) , and a Tafel slope of 52 mV dec(-1) .

213 Moreover, we achieve 10 mA cm(-2) at a low voltage of 1.44 V for 48 h in basic medi

214 The overall-water-splitting with 10 mA cm(-2) at a low voltage of 1.64 V is achieved using the

215 m cycling performance of over 480 h at 10 mA cm(-2) with high efficiency.

216 mately 0.1 V in overpotential shift at 10 mA cm(-2)) is observed for the LCO nanoparticles, where the

217 res can deliver a current density of 37.2 mA cm(-2) at an overpotential of 70 mV, which is 9.7 times

218 to achieve high sensitivity (2.4 +/- 0.24 mA cm(-2) mM(-1)) for H2O2 oxidation.

219 ent density in PEC water splitting over 5 mA cm(-2) before the dark current onset, which originated f

220 ty of 3.72 mAh cm(-2) is achieved at 5.50 mA cm(-2) on the quinonoid imine-doped graphene based elect

221 rrent at 50 mV s(-1) is 825, 615, and 550 mA cm(-1), respectively, which is significant dominated by

222 A photocurrent of over 6.8 mA cm(-2) and an accordingly high incident photon-to-curren

223 -circuit current density (J SC ) of 17.92 mA cm(-2) .

224 t current density (Jsc, from 32.5 to 37.0 mA/cm(2)).

225 e surface, yields current densities of 10 mA/cm(2) at an overpotential of 177 mV, 500 mA/cm(2) at onl

226 /cm(2) at an overpotential of 177 mV, 500 mA/cm(2) at only 265 mV, and 1,705 mA/cm(2) at 300 mV, with

227 the highest performance observed at 17.6 mA/cm(2) of photocurrent and 7.5% PCE for a cosensitized de

228 V, 500 mA/cm(2) at only 265 mV, and 1,705 mA/cm(2) at 300 mV, with high durability in alkaline electr

229 A high areal specific capacity of 3.72 mAh cm(-2) is achieved at 5.50 mA cm(-2) on the quinonoid im

230 ult, we demonstrate capacities of over 9 mAh cm(-2)areal , which is a 35-fold increase in capacity co

231 e/discharge cycles and a capacity of 1.2 mAh/cm(2) in a carbonate-based electrolyte.

232 odes with areal sulfur loadings up to 8.1 mg cm(-2).

233 ectrode with a high sulfur loading of 3.3 mg cm(-2) .

234 ulose with an areal loading higher than 3 mg cm(-2) achieve an overall specific capacity higher than

235 sulfur loading and content as high as 46 mg cm(-2) and 70 wt% with an electrolyte/sulfur ratio of as

236 ion is maintained at the lowest level (30 mg.cm(-2)).

237 ), high porosity (99.6%), light weight (5 mg/cm(3)) and narrow pore size distribution ( 2 to 5 nm), t

238 s C with a low platinum loading of 0.09 mgPt cm(-2), corresponding to a platinum utilization of 0.13

239 duct) due to the CT procedures was 1,581 mGy/cm (range, 379-2,686 mGy/cm).

240 dures was 1,581 mGy/cm (range, 379-2,686 mGy/cm).

241 al photoresponse of approximately 860 microA cm(-2) , a fivefold improvement over the best previous c

242 corresponds to a polarization of 100 microC cm(-2) , 20% larger than that of the bulk PbTiO3 .

243 The specific capacitance was 0.45 microF cm(-2) at 20 Hz, which is around 26 times higher than th

244 shold is found to be approximately 10 microJ cm(-2) , about two times less than the lowest value ever

245 nd 10 Hz with 10% duty cycle), PUT with 4 mJ/cm(2) and 6 mJ/cm(2) laser fluence induced 51% (p = 0.00

246 0% duty cycle), PUT with 4 mJ/cm(2) and 6 mJ/cm(2) laser fluence induced 51% (p = 0.001) and 37% (p =

247 high sensitivity of 12.044microA (ng per mL cm(-2))(-1) with a response time of 5min.

248 ed excellent sensitivity (90.14microA/(U/mL)/cm(2)) with a detection limit of 0.00113UmL(-1) concentr

249 VT of a 49-y-old male HAB was 7.5 +/- 1.4 mL/cm(3) compared with 4.6 +/- 1.4 mL/cm(3) of a sex- and a

250 /- 1.4 mL/cm(3) compared with 4.6 +/- 1.4 mL/cm(3) of a sex- and age-matched MAB.

251 ted unprecedented sensitivity of 37.66 Hz/mM.cm(2) and a linear range of 1 to 20 mM.

252 tection limit of about 10(4)-10(5) molecules cm(-3).

253 7 Omega (2.49 microOmega m(2) or 24.9 mOmega cm(2) ) and large specific capacitance, is among the hig

254 bination of high proton conductivity (326 mS cm(-1) at 80 degrees C) and superior mechanical properti

255 n exceptionally high conductivity of 1.46 mS cm(-1) at 25 degrees C and enhanced moisture stability.

256 ionic photoresponse of approximately 100 muA/cm(2) and approximately 1 mV under 40 Suns equivalent ex

257 nd high spontaneous polarization ( 63.3 muC.cm(-2)).

258 tedly low pump fluences of less than 400 muJ cm(-2).

259 io-frequency electric field sensing of 5 muV cm(-1) Hz(-1/2).

260 m(3) and a surface power density of 89.4 muW/cm(2) using Shewanella oneidensis as a model biocatalyst

261 e provides a volume power density of 745 muW/cm(3) and a surface power density of 89.4 muW/cm(2) usin

262 Under 325 nm 2.30 mW cm(-2) UV illumination and at a -0.45% compressive strai

263 imum power densities of 143, 196, and 325 mW cm(-2) at 500, 550, and 600 degrees C, respectively.

264 performance, with power density up to 680 mW cm(-2) at 80 degrees C with a low platinum loading of 0.

265 o (an estimated) several hours at 50 K, 1 mW/cm(2).

266 , from less than a second at 12.5 K, 100 mW/cm(2) to (an estimated) several hours at 50 K, 1 mW/cm(2

267 er light 753 nm with a fixed power of 150 mW/cm for 22 min 15 s) or active surveillance.

268 removal and 30-minute irradiation with 3 mW/cm(2) ultraviolet A light).

269 ith high volumetric energy density (36.1 mWh cm(-3) ) are fabricated via a facile and continuous meth

270 energy density of 2.58 mWh g(-1) or 3.6 mWh cm(-3), high tensile strength of over 1000 MPa, and bear

271 impedance, from 1,710 Omega cm(2) to 1 Omega cm(2), was observed at room temperature, effectively neg

272 ic electrical resistivity, over 10(11) Omega cm.

273 e of interfacial impedance, from 1,710 Omega cm(2) to 1 Omega cm(2), was observed at room temperature

274 is on the order of rho approximately 1 Omega.cm, while being essentially temperature independent.

275 4), diameter of the largest tumour (1.07 per cm increase [1.04-1.11]; p<0.0001), log alpha-fetoprotei

276 pulmonary artery side branches <300 mum per cm vessel (3.8 +/- 1.1 vs. 1.8 +/- 1.1; p = 0.010) and n

277 o our hospital and counted pollen number per cm(2) after stained by Calberla solution and then classi

278 h 2 MeV protons, a fluence of 10(16) protons/cm(2) was necessary to induce a significant charge trans

279 transport behavior, with sigmaRT near 0.04 S cm(-1) and Eact = 0.05 eV, is more consistent with a Mot

280 and the highest one ever reported of 0.17 S cm(-1) at 75 degrees C, under 97% relatively humidity, a

281 d a proton conduction value of over 10(-3) S cm(-1) at 25 degrees C and 40% RH, a very high proton co

282 r than other members of the series (10(-3) S cm(-1) versus 10(-4) S cm(-1)).

283 high proton conductivity of 3.40 x 10(-4) S cm(-1) at 25 degrees C and the highest one ever reported

284 the series (10(-3) S cm(-1) versus 10(-4) S cm(-1)).

285 osts electrical conductivity to up to 0.62 S cm(-1) , among the highest conductivities that have been

286 lectrical conductivity to be 11,000-15,000 S/cm, substantially higher than the only earlier reported

287 ivity values up to sigma = 1.4(7) x 10(-2) S/cm (Ea = 0.26(1) cm(-1)) and 1.0(3) x 10(-3) S/cm (Ea =

288 ractically useful conductivities of 10(-2) S/cm at room temperature (RT).

289 (Ea = 0.26(1) cm(-1)) and 1.0(3) x 10(-3) S/cm (Ea = 0.19(1) cm(-1)) in its solvated and desolvated

290 i(+) conductivity improves to 4.8 x 10(-4) S/cm.

291 4 x 10(-5), 1.8 x 10(-5), and 8.8 x 10(-7) S/cm.

292 d thermal (>65 W/m-K) and electrical ( 700 S/cm) conductivities, as well as high thermoelectric power

293 r resistance below the mean (1,011 dynes x s/cm(5) ) revealed no effect of rifaximin.

294 ansistors and photodetectors at wafer scale (cm(2)) without postgrowth transfer or alignment steps.

295 ormula: see text]m(2) to [Formula: see text] cm(2) Electron microscopy reveals the excellent quality

296 ford high-resolution images at depths in the cm range.

297 l was achieved at applied potentials of 20 V.cm(-1), within 120 s of stimulation, using 0.1 M iron (i

298 ires a field strength of approximately 100 V/cm, yet it efficiently recovers proteins and nucleic aci

299 rated power density of approximately 0.13 W cm(-2) at a constant current density of 0.15 A cm(-2) wi

300 5 nM) of AuNRs and the PPTT laser power (2 W/cm(2)) to achieve maximal induction of apoptosis.