ライフサイエンスコーパス: kV

1 kV) to 140.93, 157.13, and 172.94 um (at 1.0 kV) to 145.03, 191.34, and 212.84 um (at 1.5 kV), respec

2 ereas the other half utilized PF (single 2.0 kV application with a proprietary waveform).

3 lesions were performed with PFA (single 2.0 kV application) with targeted levels of CF: low, 5 to 15

4 s used to deliver bipolar, biphasic PFA (2.0 kV) lesions guided by electroanatomical mapping, fluoros

5 e heating occurs at voltages of at least 2.0 kV.

6 were performed by applying a voltage of 25.0 kV and a detection at 200.0 nm.

7 flow) with pulsed electric fields (PEF: 3.0 kV/cm, 300 kJ/kg for head/backbones, 124.8 kJ/kg for vis

8 sure of the 20 h grown culture to PEF of 5.0 kV/cm and 20 mus pulse width, accumulation of magnesium

9 The higher the ac voltage applied (max. 9.0 kV) to the plasma air purifier, the higher the mass of t

10 , and Mycobacterium smegmatis (5.56 +/- 0.08 kV/cm) have been successfully characterized.

11 such as Escherichia coli BL21 (3.65 +/- 0.09 kV/cm), Corynebacterium glutamicum (5.20 +/- 0.20 kV/cm)

12 ple plug lengths for 5-FAM and FL under 20.1 kV for 60 min were experimentally estimated as 836 and 7

13 3% when the positive phase was 150 ns at 3.1 kV/cm, and the negative phase was 800 ns at 0.2 kV/cm.

14 Measured plate heights at 1 kV/cm applied electric field were 0.77, 1.33, and 1.42 m

15 rn, accounts for the high electric field (>1 kV/m) that can be achieved even with a low applied volta

16 igomers start separating at fields of just 1 kV/cm (4 Td), or ~5% of those typical for FAIMS.

17 n applying electric fields on the order of 1 kV/cm to the BaTiO3 substrate, corresponding to magnetoe

18 We find that a THz field of strength 1 kV cm(-1) can produce a high-sideband spectrum of about

19 trains, or ramps, at rates from 10 V/s to 1 kV/s, to a maximum transmembrane potential of +/-1000 mV

20 With 1 kV applied to the microchip during dispensing, the relat

21 under reverse polarity at pH 3.5 using 5-10 kV in less than 20 min.

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

23 ect THz pulses with peak fields as low as 10 kV cm(-1).

24 : the required voltage accuracy is 5 V in 10 kV, and the mechanical precision is 1 mm in 5 cm.

25 s (including reducing coercive fields to <10 kV cm(-1) and improving switching times to <5 ns for a 2

26 ten needle discharges a high voltage of - 10 kV at the front of the grounded mesh structure.

27 dodecyl sulphate (SDS) including sample (-10 kV, 20 s) was introduced in this MEEKC system and this y

28 ed by micropulsed electric fields of some 10 kV.cm(-1) amplitude and ampere-transient currents.

29 een observed with large field strengths (~10 kV cm(-1)), an obstacle for technological applications.

30 ing peak-to-peak potentials of +/-1 to +/-10 kV, the paper-based devices produced both volume and sur

31 For the 10-kV instrument, computed isotopic compositions were indep

32 For the 10-kV instrument, sample requirements for standard deviatio

33 as 29.1 (80 kV), 21.2 (80 kV), and 11.5 (100 kV).

34 (either 140 and 80 kV [n=44] or 140 and 100 kV [n=108], with tin filtration at 140 kV).

35 CT images were acquired at 100 kV and 200 mA using a fast-pitched helical scan mode cov

36 afer, using electron beam lithography at 100 kV and polymethyl methacrylate (PMMA) resist at differen

37 om a microfocus X-ray source operated at 100 kV was measured with thin film photovoltaic cells (TFPCs

38 ct-charged voltage plasma focus (PF), at 100 kV, 1 MA peak current.

39 patients underwent both dual-energy CT (100 kV and Sn140 kV, where Sn indicates the use of a 0.4-mm

40 <200 lb [90 kg], 80 kV; >200 lb [90 kg], 100 kV).

41 A tube potential of 100 kV was used in 97 patients (90.6%), single-volume acquis

42 For a maximum ambient electric field of 100 kV/m typically measured in thunderclouds, such field enh

43 eneration dual-source CT system at 80 or 100 kV (n = 15 for each).

44 ng 30 volumes with identical parameters (100 kV, 200 mAs, 0.5 sec rotation time).

45 uired using very low tube voltage (80 to 100 kV) and current (150 to 210 mA) and was reconstructed wi

46 cial bushings, however, are limited to ~ 100 kV, and exceeding this limit has proven to be difficult.

47 or 70 kV for less than 26 kg/m(2) versus 100 kV for 26-30 kg/m(2).

48 (70 kV: 14.3-17.6 vs 80 kV: 7.1-12.9 vs 100 kV: 9.8-12.9; P < .0497) than those acquired with the ot

49 < .0001), respectively, for the 80- and 100-kV CT angiography protocols than for the 70-kV CT angiog

50 For the 80- and 100-kV protocols, 80 mL of contrast material was injected, v

51 a matched load when fully charged to +/- 100-kV.

52 Mean kilovoltage in all facilities was 101 kV.

53 12-ns stimuli at 4.1-11 kV (3.3-8.8 kV/cm) evoked APs similarly to conventional

54 hese separation conditions (249 microA at 11 kV) is extremely high by capillary electrophoresis (CE)

55 econdary ion mass spectrometric analysis (12 kV Ga+ primary ion beam), and through X-ray photoelectro

56 s were studied: group 1 (n=4), 2000 SW at 12 kV to one pole and 2000 SW at 24 kV (standard) to the op

57 nction, was not significantly affected at 12 kV, was transiently reduced at 18 kV, and was reduced fo

58 group 4 (n=8), same as group 3 except 100 12-kV SW pretreatment.

59 group 2 (n=6), same as group 1 except 500 12-kV SW pretreatment; group 3 (n=8), 500 12-kV, 2000 stand

60 12-kV SW pretreatment; group 3 (n=8), 500 12-kV, 2000 standard SW, all to the same pole; and group 4

61 ed with 3-mm-thick sections, pitch of 1, 120 kV, and 180-220 mA, after injection of 150 mL nonionic c

62 hickness, 2.5-mm interval, pitch of 1.3, 120 kV, 240 mA, and 0.5-second rotation time.

63 -120 keV) x-ray beams, polyenergetic (40-120 kV, tungsten anode) x-ray spectra, and polyenergetic mam

64 re derived for exposures at 80, 100, and 120 kV.

65 Representative values of ED/DLP at 120 kV were 2.2 microSv/mGy x cm (head scans), 5.4 microSv/m

66 tive tube potentials relative to SSDE at 120 kV were less than 5%.

67 ty patients underwent four-section CT at 120 kV, 170 mAs, and 4 x 1-mm collimation.

68 or thoracic CT examinations performed at 120 kV.

69 o 15 patient data sets were used, all at 120 kV.

70 nts referred for thoracic CT, spiral CT (120 kV, 292 mA) was performed with 1-second (n = 45) or 0.75

71 atients (group 2) acquired in a 16-MDCT (120 kV and filtered back-projection).

72 T examinations performed in 83 patients (120 kV, 70 quality reference mAs [QRM]) were collected betwe

73 were acquired at the following settings: 120 kV, 300 mA, pitch of 1.35:1, collimation of 8 x 1.25 mm,

74 were acquired at the following settings: 120 kV, 50-150 mA, cine duration of 1 breathing cycle plus 1

75 scans at five tube potentials other than 120 kV.

76 nd for general diagnostic x-ray beams to 120 kV.

77 onounced at lower accelerating voltages (120 kV versus 200 kV) in both the metals.

78 MDCT parameters were 120 kV, 120 mA/s, collimation 12x0.75, and spatial resolutio

79 In a 120-kV standard PCD CT scan of a 40-cm phantom, VMI iodine C

80 Compared with standard 120-kV scans, kV-independent and tin filter scans showed exc

81 n CACS estimation compared with standard 120-kV scans, with large reductions in radiation dose.

82 ired with an ultra-low dose CT (32-MDCT, 130 kV, tin filter and iterative reconstruction).

83 at 24 combinations of four kilovolt (80-140 kV) and six milliampere (200-300 mA) levels.

84 original polychromatic images at 80 and 140 kV and six series of virtual monochromatic spectral imag

85 was scanned with dual-energy CT (80 and 140 kV) by using a dual-source multi-detector row CT scanner

86 T scanner was used for imaging at 80 and 140 kV, and a three-material decomposition algorithm was use

87 iginal polychromatic images at 80 kV and 140 kV.

88 y images acquired with 80, 100, 120, and 140 kV.

89 a significant difference with images at 140 kV (mean energy, 92 keV).

90 d 100 kV [n=108], with tin filtration at 140 kV).

91 , whilst the CNR for gold was highest at 140 kV.

92 s included near constant radiation dose (140 kV and varied tube current, confirmed by using the above

93 refoot underwent noncontrast DECT (80 kV/140 kV) and MRI between October 2020 and February 2022.

94 scanning protocol (tube voltage, 120 or 140 kV; collimation, 120 x 0.2 mm; 100 mL of iopromid; no sp

95 At the highest settings (140 kV and 300 mA), the detection threshold size (ie, the si

96 D values for tube voltages from 80 kV to 140 kV in steps of 20 kV for the following examinations: hip

97 for body scans, the increase from 80 to 140 kV increased the ratio of ED to DLP by approximately 25%

98 The setup was optimized to allow -15 kV to be applied to the device for high efficiency and r

99 uration and electric fields between 4 and 15 kV/cm, intracellular calcium increased 200-700 nM, respe

100 high potential difference (approximately 15 kV).

101 The separation was performed at 15 kV under reverse polarity and completed within 10 min.

102 tching rates at high voltage (~ 20-kHz at 15-kV) resulting from the intrinsically limited charge carr

103 cros-60 ns, electric field intensities 3-150 kV/cm) to Jurkat cells suspended in physiologic buffer c

104 ents underwent dual-energy CT (90 kV and 150 kV with a tin filter) and 3-T magnetic resonance (MR) im

105 one attenuation at 70, 90, 110, 130, and 150 kV.

106 llector distance, 0.6 ml/h flow rate, and 18 kV applied voltage) significantly outperforms alternativ

107 esponse of 34.96 mV/pH when fabricated at 18 kV and CeO(2) reaching a peak H(2)O(2) sensitivity of 1.

108 sions obtained from conjugate produced at 18 kV for 5 min, which had the most stability after 14 days

109 cted at 12 kV, was transiently reduced at 18 kV, and was reduced for the duration of the experiment a

110 the heel, with a total of 1500 shocks at 18 kV.

111 180 mm) tested at the applied voltage of 18 kV, experimental total particle collection efficiencies

112 cm, and the negative phase was 800 ns at 0.2 kV/cm.

113 Combined with 1.2 kV/cm and a short effective length (15 cm to the UV dete

114 c field strengths in the nanochannels (0.2-2 kV/cm) and enabling rapid dispensing and analysis (10-10

115 t voltages were used (1.0, 1.4, 2.0, and 2.2 kV).

116 the voltage of the DBDI source from 0 to 3.2 kV, the classes of detected metabolites can be shifted f

117 An electric field of 0.5-2 kV/cm applied between the microsprayer and a separation

118 63.7 J), activation electric fields (-921.2 kV cm(-1)mol(-1)), and electrical activation energy (12.

119 mental conditions existing between 1.6 and 2 kV/cm.

120 um, 65 pL) fall on a steel needle held at +2 kV where they subsequently form a spray that is directed

121 nipolar) under a very low applied field of 2 kV mm(-1), resulting in record-breaking piezoelectric co

122 animals received 8 PFA applications/site (2 kV, multispline catheter), and 4 animals received 6 clus

123 High field strength (+2 kV/cm) enables rapid second-dimension separations in whi

124 The application of a PEF treatment (2 kV/cm; 11.25 kJ/kg) to the olive paste significantly inc

125 ), Corynebacterium glutamicum (5.20 +/- 0.20 kV/cm), and Mycobacterium smegmatis (5.56 +/- 0.08 kV/cm

126 range of electric field amplitudes (0.05-20 kV/m).

127 th 2% osmotic flow modifier (pH 9.0) and -20 kV applied potential for baseline resolution of each ars

128 ation was studied, and a CE separation at 20 kV was found to be optimal for the present setup.

129 s electrospraying and spinning process at 20 kV, nanoencapsulated anthocyanin was immobilized on ethy

130 cept the voltage selection was reduced by 20 kV with adaptation of the tube current to ensure a 50% r

131 voltages from 80 kV to 140 kV in steps of 20 kV for the following examinations: hip (femur), knee, an

132 In studies up to 20 kV, this materials design provides a sufficient dielectr

133 creasing E(D) from 12 to 16 or from 16 to 20 kV/cm is equivalent to heating the (N2) gas by approxima

134 rototype operation at multi-10s of kW and 20-kV, 125-kHz in a bulk conduction transistor-like device

135 -in electric fields in films as large as 200 kV/cm.

136 we used cryogenic electron microscopy at 200 kV to determine structures of a folate-specific ECF tran

137 te (10(3)), and delta-MnO(2) (<10(3)) at 200 kV.

138 a Mach-Zehnder geometry in an unmodified 200 kV transmission electron microscope.

139 wer accelerating voltages (120 kV versus 200 kV) in both the metals.

140 ld by approximately 35% over the previous 21 kV/cm provides similar or better resolution (with resolv

141 llector distance, 1.2 ml/h flow rate, and 22 kV applied voltage, which display larger diameters, redu

142 reatments with 1-20 unipolar NEFO, at 9.6-24 kV/cm, 10 Hz, the rate and amount of YP uptake were cons

143 00 SW at 12 kV to one pole and 2000 SW at 24 kV (standard) to the opposite pole; group 2 (n=6), same

144 ced for the duration of the experiment at 24 kV.

145 vity of 1.03 uA/uM/cm2 when fabricated at 24 kV.

146 g received 2000 shock waves at 12, 18, or 24 kV to the lower pole calyx of one kidney.

147 hock wave energy was increased from 12 to 24 kV.

148 Each pig received 2000 shock waves, 24 kV, or sham SWL to the lower pole calyx of one kidney.

149 e preconcentrator successfully withstood 240 kV/m for 100 min that was required for the microfluidic

150 concentration (1-2% w/v) and voltage (21-25 kV) were varied with VC (0.25-0.75 w/w Cs).

151 alytes were separated at 12 degrees C and 25 kV with a background electrolyte of 25 mM borate buffer

152 Cold plasma at 25 kV/10 min and steam at 100 degrees C/6 min achieved >=99

153 Cold plasma at 25 kV/10 min preserved the color and proximate composition

154 PEF treatment at 25 kV/cm at 50 degrees C denatures Pru p 3.

155 animals treated with nsPEF (750, 200-ns, 25 kV/cm, 2 Hz) with animals were tumors were surgically re

156 perature of 20 degrees C and a voltage of 25 kV (normal mode) were applied.

157 dodecyl sulphate at an applied voltage of 25 kV.

158 PME inactivation level after the PEF (25.26 kV/cm-1206.2 mus) and HP (90 degrees C-20s) treatments w

159 PEF treatments were applied at 20 or 26 kV cm(-1) for 34 mus with or without pre-heating of milk

160 a rhodium target and rhodium filter with 29 kV, 50 mAs, and seven acquisition protocols.

161 ectric field strengths of approximately 13.3 kV/cm and approximately 40 kV/cm for PEF and HVED treatm

162 parameters included field strength (0.1-3.3 kV/cm), pulse length (0.05-20 ms), number of pulses (1-1

163 At 400-600 V (2.9-4.3 kV/cm), the split-dose treatments increased the ablation

164 for 4 s and separated using a potential of 3 kV and a background running electrolyte (BGE) consisting

165 power of R(P) > 80 at low drift voltage of 3 kV and short drift length of 50 mm can be achieved indep

166 to 2 microL/min for an applied voltage of 3 kV at a pH of 6.8.

167 ically injected by applying a potential of 3 kV for 4 s and separated using a potential of 3 kV and a

168 nt design for a maximum applied voltage of 3 kV.

169 (-1) trypsin is electrosonically sprayed (-3 kV) from a homemade setup to produce tiny (~9 um) microd

170 ble figures for the second instrument were 3 kV, 0.5 mL of He/min, and 14000 molecules/ion.

171 Comparable requirements for the 3-kV instrument were 900 and 36 pmol.

172 earities of <0.04%/V were observed for the 3-kV system.

173 Of the various treatments, 3-kV plasma exposure for 10min yielded the best results.

174 sodium tetraborate 40 mM at a pH of 9.4, 30 kV, 25 degrees C, 10s of hydrodynamic injection (0.5 psi

175 obtained over the full voltage range of 5-30 kV, with no requirement for pressurization.

176 ited a remarkable improvement (4.78 %) at 30 kV for 6 min compared to PPI (3.23 %).

177 alonyl CoA) were completely separated at -30 kV in a 100 mM NaH2PO4 running buffer containing 0.1% be

178 Runtime in a 40 cm capillary (30 kV) was 35 min for elution of all products down to the 2

179 phate buffer at pH 2.00 and a voltage of -30 kV.

180 te without arcing at voltages higher than 30 kV.

181 etic 50-Hz fields with strengths of up to 30 kV.m(-)(1) and 2.55 mT.

182 consecutive runs at the highest voltage (30 kV) without thermostating and pressurization.

183 nducted on images recorded at 4 K with a 300 kV field emission source, by combining data from four he

184 spectrometer (SIMS) was coupled to a +/- 300 kV single-stage accelerator mass spectrometer (SSAMS).

185 ing - that Hammerhead operates stably at 300 kV with dark current below 10 muA.

186 on that exceeds the 1.9-pm wavelength of 300 kV electrons.

187 ls were exposed to high intensity (up to 300 kV/cm) nanosecond (10-300 ns) pulsed electric fields (ns

188 The coercive field of DJP(n=2) (0.34 kV/cm) is lower than that for the n = 1 homologue (AMP)P

189 (PB) cells were passed through PEFs at 1.35 kV/cm to 1.4 kV/cm, resulting in 3- to 4-log tumor cell

190 he n = 1 homologue (AMP)PbI(4) (DJP(n=1),0.4 kV/cm).

191 sinusoidal waveform with an amplitude of 1.4 kV and mobility analyzed in a 19 mm long drift region.

192 ere passed through PEFs at 1.35 kV/cm to 1.4 kV/cm, resulting in 3- to 4-log tumor cell depletion by

193 A single 14.4 kV/cm unipolar NEFO caused a 1.5-2 times greater increas

194 lated with conventional pulses (CPs; 0.5-2.4 kV/cm, 1 ms) or nsPEF (10-80 kV/cm, 4 ns).

195 A PEF treatment of 3.4 kV/cm and 105 mus (35 pulses of 3 mus) resulted in the h

196 wo-temperature theory, and raising E(D) by 4 kV/cm augments heating by approximately 15-30 degrees C

197 cid dissolved in water is electrosprayed (-4 kV) by using nitrogen gas at a pressure of 120 psi to fo

198 applied field strengths of at least up to 4 kV x cm (-1).

199 of a high separation voltage (i.e., up to 4 kV) together with organic modifiers (e.g., alcohols, ace

200 ure helium gas is ionized by high voltage (4 kV) and high frequency (6 kHz).

201 pproximately 13.3 kV/cm and approximately 40 kV/cm for PEF and HVED treatments were used, respectivel

202 of two 25-mum Al wires on a compact L-C (40 kV, 200 kA and 200 ns) generator, and the time integrate

203 to the introduction of new higher energy (40 kV) gas cluster ion beams (GCIBs), time-of-flight second

204 For a 1-ms, 40 kV/m pulse, electroporation consists of three stages: ch

205 a handheld Bruker Tracer III- SD XRF with 40 kV of voltage and a 30muA current.

206 heterogeneous in images obtained with a 400-kV electron cryomicroscope.

207 entations of particles in focal pairs of 400-kV, spot-scan micrographs are determined and iteratively

208 Using 400-kV spot-scan images of the bacteriophage P22 procapsid,

209 caused by nanoscale electric fields of ~487 kV/cm between photogenerated free carriers in the device

210 d from 105.19, 123.67, and 135.55 um (at 0.5 kV) to 140.93, 157.13, and 172.94 um (at 1.0 kV) to 145.

211 kV) to 145.03, 191.34, and 212.84 um (at 1.5 kV), respectively.

212 2)O: ACN) mixture was electrosprayed at +1.5 kV, and the reaction products were analyzed using a mass

213 in stable electrospray at approximately 1.5 kV.

214 Electric fields as high as 1.5 kV/cm were applied in these microchips, and >300 CE runs

215 , 6 psi (0.414 bar); capillary voltage, +2.5 kV; fragmentor voltage, 85 V), baseline enantioseparatio

216 s treated with a single 300-ns pulse of 25.5 kV/cm, Tmem16f expression knockdown and TMEM16F-specific

217 y treated: subjected to PEF (5 pulses of 3.5 kV cm(-1)) (PEF); thermally treated (70 C for 10 min) (T

218 PANC-1 cells were observed in ESI mode (3.5 kV) and an additional 49 compounds in onion cells and 73

219 ds in PANC-1 cells were detected in ESI (3.5 kV)-DBDI (2.6 kV) hybrid mode.

220 litudes and frequencies: 7 kV/10 kHz and 8.5 kV/14 kHz.

221 ithin the device, which generates up to +/-5 kV dc voltage to ignite a corona discharge plasma in air

222 V, 200 ns pulses at 2 kHz and 60-nsPEF of 50 kV/cm at 1 Hz, the synergistic effects on pancreatic can

223 nized water in the presence of a strong (0.6 kV/cm) electric field.

224 the presence of a strong electric field (0.6 kV/cm).

225 d at high average field strengths (up to 1.6 kV/cm) without encountering the field-dependent loss of

226 ells were detected in ESI (3.5 kV)-DBDI (2.6 kV) hybrid mode.

227 lls, a train of 120 pulses (300 ns, 20 Hz, 6 kV/cm) decreased cell survival to 34% compared with 51%

228 lectric field pulse sequences of less than 6 kV/cm induce large, reversible, and bistable remanent st

229 By raising the waveform amplitude to 6 kV, we enabled high FAIMS resolution using solely N(2) a

230 metry (FAIMS) analyses was doubled to E > 60 kV/cm.

231 allowed electric field intensity (E) over 60 kV/cm, or about twice that in previous devices with >0.5

232 aps permit higher E: here, we established 61 kV/cm in N(2) using microchips with 35 microm gaps.

233 lasmid DNA under 100 Ohms resistance and 1.7 kV/cm voltage.

234 cts of pulsed electric fields (PEF) (1.4-1.7 kV/cm, 653-695 kJ/kg) and heating (60 and 80 degrees C f

235 A high responsivity Rv of 15.5 and 2.7 kV/W and a low NEP of 0.58 and 10 pW/Hz(0.5) were obtain

236 thality in nsEP-treated cells (300 ns, 1.8-7 kV/cm, 50-700 pulses).

237 However, the threshold amplitude was about 7 kV/cm for both NEFO waveforms.

238 ons of voltage amplitudes and frequencies: 7 kV/10 kHz and 8.5 kV/14 kHz.

239 hat in vitro nsPEF (20-200, 200-ns pulses, 7 kV/cm, 2 Hz) caused a rapid dose-dependent cell death wh

240 third-generation dual-source CT system at 70 kV (n = 15) or with a second-generation dual-source CT s

241 ch coronary dual-source CT angiography at 70 kV results in robust image quality for studying the coro

242 ead, a medium effect size was observed at 70 kV; however, the mean absolute difference in WED was sma

243 ired with 70 kV was significantly higher (70 kV: 14.3-17.6 vs 80 kV: 7.1-12.9 vs 100 kV: 9.8-12.9; P

244 ltage was based on body mass index: 80 or 70 kV for less than 26 kg/m(2) versus 100 kV for 26-30 kg/m

245 nary CT angiography studies acquired with 70 kV was significantly higher (70 kV: 14.3-17.6 vs 80 kV:

246 -kV CT angiography protocols than for the 70-kV CT angiography protocol.

247 terial was injected, versus 45 mL for the 70-kV protocol.

248 iments, 6-stage TITAN is tested up to +/- 70-kV charge voltage which delivers a peak power of 330-GW

249 switches, could generate ~ 600-kA and ~ 700-kV across a ~ 0.9-Omega matched load when fully charged

250 s, very low ESI voltages (typically 1.4-1.75 kV) suffice for stable ESI, which eventually allows for

251 s, i.e. Yellow Solar, the application of 0.8 kV/cm resulted in a higher total carotenoid content in t

252 Electric polarization at 52.8 kV cm(-1) normal to the film plane increases the photocu

253 Applying 2 mus pulses at 7-8 kV/cm and 0.1% duty cycle results in 80-100% bacteria in

254 12-ns stimuli at 4.1-11 kV (3.3-8.8 kV/cm) evoked APs similarly to conventional stimuli (100

255 nanosecond electrical pulses between 1 and 8 kV in magnitude.

256 electrical breakdowns up to 10(-2) hPa at 8 kV acceleration voltage.

257 um gas that is produced by a high-voltage (8 kV) and high-frequency (6 kHz) power supply.

258 ed of a microchip, microchip holder, two 0-8-kV high-voltage power supplies, a high-voltage switch, a

259 imal tube potential, iodine CNR was 29.1 (80 kV), 21.2 (80 kV), and 11.5 (100 kV).

260 s (CPs; 0.5-2.4 kV/cm, 1 ms) or nsPEF (10-80 kV/cm, 4 ns).

261 ntial, iodine CNR was 29.1 (80 kV), 21.2 (80 kV), and 11.5 (100 kV).

262 ) rather than air, increasing voltage (60-80 kV) and reducing sample volume (30 mL-10 mL).

263 Here, we show that irradiation with an 80 kV electron beam can selectively remove monolayers in fe

264 hy in the excretory phase (either 140 and 80 kV [n=44] or 140 and 100 kV [n=108], with tin filtration

265 no significant differences with images at 80 kV (mean energy, 54 keV).

266 d on the original polychromatic images at 80 kV and 140 kV.

267 ed by reaction with XeF2 were obtained at 80 kV in an aberration-corrected transmission electron micr

268 oise ratio (CNR) of iodine was highest at 80 kV, whilst the CNR for gold was highest at 140 kV.

269 and forefoot underwent noncontrast DECT (80 kV/140 kV) and MRI between October 2020 and February 202

270 tivated via the ultrahigh electric field (80 kV/mm) leads to large polarization and superior energy s

271 o obtain ED values for tube voltages from 80 kV to 140 kV in steps of 20 kV for the following examina

272 as based on body weight (<200 lb [90 kg], 80 kV; >200 lb [90 kg], 100 kV).

273 d pigs over 180 seconds by using routine (80 kV, 160 mAs) and one-tenth (80 kV, 16 mAs) dose levels.

274 ve isotropic (0.6 mm) diagnostic CT scan (80 kV, 165 mAs) and a subsequent PET scan (2 min per bed po

275 g routine (80 kV, 160 mAs) and one-tenth (80 kV, 16 mAs) dose levels.

276 significantly higher (70 kV: 14.3-17.6 vs 80 kV: 7.1-12.9 vs 100 kV: 9.8-12.9; P < .0497) than those

277 An 80-kV abdominal CT can be performed with appropriate diagno

278 mic (500 mum), the U(50) value reaches to 86 kV, which is enhanced about 21.13% in comparison with th

279 High PEF input (112 kJ/kg, 1.875 kV/cm and 100 Hz) yielded the highest total lipid (16.2%

280 oating (500 mum), a higher U(50) value of 88 kV is obtained.

281 maximum measured intra-crystal field of 10.9 kV/m, signal duration and detected frequency content whi

282 Employing ns-APPJ powered by 9 kV, 200 ns pulses at 2 kHz and 60-nsPEF of 50 kV/cm at 1

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

284 Treatment with HVACP in air at 90 kV for 120 s inactivated 1.30 log(10) of ST2.

285 All patients underwent dual-energy CT (90 kV and 150 kV with a tin filter) and 3-T magnetic resona

286 nner for axial volumetric head CT, adjusting kV and mAs based on attenuation data from scout images.

287 V) curves were modeled exponentially by P=ae(kV)+b and logarithmically by P=-Sln[(Vm-V)/(Vm-V0)], whe

288 arameter, alpha from 28 +/- 4 to 47 +/- 5 cm/kV.

289 ose Reduction, Low-Dose CT Scan, Tin Filter, kV-Independent Supplemental material is available for th

290 ed with the use of high operating voltages (>kV) and corresponding failure due to dielectric breakdow

291 res created by low intensity exposure to low kV electrons.

292 , of leaf wax crystals was evident under low-kV scanning electron microscopy after each drying event.

293 potentials required, in the order of tens of kV or more.

294 m range at kHz repetition rates, and tens of kV/cm at oscillator repetition rates.

295 Compared with standard 120-kV scans, kV-independent and tin filter scans showed excellent cor

296 erwent both dual-energy CT (100 kV and Sn140 kV, where Sn indicates the use of a 0.4-mm tin filter) a

297 rved, and comparisons are made with standard kV paper spray (PS) ionization and nanoelectrospray ioni

298 Conclusion The kV-independent and tin filter research CT acquisition te

299 ration devices deliver voltage pulses in the kV range to the cell medium.

300 ero volt PS is applicable is very similar to kV PS and nESI, differences in the mass spectra of mixtu

301 determine the effects of shock wave voltage (kV) on lesion size and renal function induced by shock w