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1 requency, intensity, treatment duration, and pulse width).
2 iod of ~25 min (corresponding to 5 to 15 min pulse widths).
3 D50, and they both decreased with decreasing pulse width.
4 threshold showed a similar relationship with pulse width.
5 expand existing frequency resources based on pulse width.
6 nnabidiol and interference #1 at 70 mus gate pulse width.
7 g cascade creates a system that is robust to pulse width.
8  GnRH pulse, and this reduces sensitivity to pulse width.
9 nd broadening, and by reducing the injection pulse width.
10 f 0.5 msec is more efficient than the 1-msec pulse width.
11 ith the 0.5-msec pulse width than the 1-msec pulse width.
12 ith the 0.5-msec pulse width than the 1-msec pulse width.
13 the most correlated features were related to pulse-width.
14  threshold voltage was insensitive to longer pulse widths.
15 w long the waves continued, namely, on their pulse widths.
16 or better, being limited only by the optical pulse widths.
17 OG, without change in contacts, voltages and pulse widths.
18 or the complete range of clinically relevant pulse widths (0.5-100 mus) and electric fields (100-2500
19  follows: mean pacing threshold (at a 0.4-ms pulse width), 0.40 +/- 0.26 V and 0.43 +/- 0.30 V; R-wav
20 mented torques, non-linear responses to wide-pulse width (1 ms), low-intensity, variable-frequency (2
21 on of cartridge-type N2 lasers (337 nm, 4-ns pulse widths, 1-30-Hz repetition rates) more than a deca
22 a subcutaneously implanted nerve stimulator (pulse width 100 micros or 1 ms, frequency 20 or 160 Hz,
23 e active neurostimulation (frequency 180 Hz; pulse width 120 mus; amplitude 0.5 V below adverse event
24 requency (2-20 Hz), intensity (0-3.5 mA) and pulse widths (130-750 mus) over 14 months.
25 itrification and laser warming (300 V, 10 ms pulse width, 2 mm beam diameter) using a vitrification s
26          A train of 10 pacing stimuli (10-ms pulse width, 200-ms cycle length) was coupled to the sho
27  and analog switching tests with ultra-short pulse width (300 ps) was carried out.
28 proach to measuring a strong 118 MV/m narrow pulse width (~ 33 ns) electric field in the magnetically
29                  Pacing parameters including pulse-width (50, 100 ms), pulse-amplitude (2, 4, 8 mA) a
30 f live rhesus monkey eyes for five different pulse widths (7 nsec; 80, 20, and 1 psec; and 150 fsec).
31 grown culture to PEF of 5.0 kV/cm and 20 mus pulse width, accumulation of magnesium and zinc in yeast
32 urthermore, modulation of the current or the pulse width affords the ability to control the three-ste
33 er, (76 MHz repetition rate, 150 femtosecond pulse width), allowing for the visualization of individu
34   Moreover, a composite metric incorporating pulse width, amplitude, and frequency predicted therapeu
35  pulsed MW power (500 and 667 W/kg with 10 s pulse width and 20 s pulse interval resulting in an aver
36 w frequency stimulation, paired with greater pulse width and amplitude, relieved bradykinesia.
37  wall states as a function of in-plane field pulse width and amplitude.
38 e, the temporal resolution is limited by the pulse width and by the difference in group velocities of
39                                          The pulse width and frequency of the stimulation were swept
40 fore, this study investigated the effects of pulse width and intensity of nsPEF on the murine melanom
41 ferent parameters of incident light, such as pulse width and number of pulses.
42 th from 1.5 to 2.3 THz (based on the chirped pulse width and supercontinuum bandwidth), reduce signal
43 s to GES were strengthened with an increased pulse width and/or frequency of stimulation; T9-T10 spin
44 cal intravascular stimulation at 20 Hz, 4 ms pulse width, and <=20 mA.
45 Optimal PEF conditions were 10 kV/cm, 20 mus pulse width, and 50 pulses (40 kJ/kg), while the best US
46 t electrical stimulation, cycling with fixed pulse width, and cycling with adaptive adjustment of pul
47 ter sweeps of stimulation current amplitude, pulse width, and electrode configuration, and used a lin
48 ated as a function of various beam diameter, pulse width, and power conditions at visible and near-in
49 h can be modulated by varying the amplitude, pulse width, and size of the pacing vector.
50 h an increase in the pacing pulse amplitude, pulse width, and vector spacing.
51 s for different photostimulation amplitudes, pulse widths, and frequencies.
52                                 LFP (380 nm, pulse width approximately 350 fs) of 2 and 3 allowed dir
53  nm absorption obtained from the 355 nm LFP (pulse width approximately 7 ns) of 1, 2, and 4 has been
54         In this approach, microJoule pulses (pulse widths, approximately 600 ps) are focused using hi
55                  Phase-2 voltage and maximum pulse width are dependent on phase-1 pulse characteristi
56 lt in gas multiplication, where deadtime and pulse width are observed to be increasing.
57 ted with increased membrane conductance when pulse widths are microseconds rather than nanoseconds.
58       Also, the near-IR thresholds for these pulse widths are much higher than for the visible wavele
59 eatment frequency, electrode placements, and pulse width, are discussed in the light of recent eviden
60 nctionalities or performances in response to pulse width as a new capability.
61       Here, we demonstrate that high voltage pulse widths as narrow as 100 ns with a pulse-to-pulse d
62 n avalanche diodes, we demonstrate avalanche pulse widths as small as ~30 ns, 10x smaller than a pass
63 onse function (i.e., a negligible excitation pulse width) as does most current rapid lifetime determi
64 a pacing threshold up to 2.0 V at a 0.4-msec pulse width at 6 months.
65 y the storage-ring timing patterns and X-ray pulse width at synchrotron sources.
66  conductivity and modulated in real time the pulse width based on the conductivity.
67           We implemented a single-wavelength pulse-width-based method with a one-dimensional imaging
68    Reducing the sensing volume decreases the pulse width but increases the overall pulse amplitude wi
69 dth, and cycling with adaptive adjustment of pulse width by the fabricated controller.
70 ubcycle field waveforms with almost constant pulse widths can be generated without a dramatic degrada
71 spectral resolution at longer effective gate pulse widths compared to the traditional set of multiple
72  690 to 1050 nm, prechirper optics for laser pulse-width compression, resonant galvanometer for video
73 nd fixed control conditions and the adaptive pulse width control system of the fabricated controller
74 termined to be both compound and initial ion pulse width dependent.
75 drift length, voltage across drift cell, and pulse width determined the requirements for designing a
76 ations using time-gated detection and finite pulse width excitation.
77  induced by fewer, lower amplitude and short pulse width exposures may only allow extracellular calci
78 interval bipolar capture threshold at 0.5-ms pulse width for the IPL increased from 0.69+/-0.14 V at
79 n mobility spectra were studied with various pulse widths for both positive and negative ions, giving
80 epetition rate Nd:YAG laser (355 nm, <500-ps pulse widths) for atmospheric pressure MALDI-QqTOFMS, an
81 ponses, over a range of pulse amplitudes and pulse widths, for 21 cell types spanning the inner two l
82 depends on stimulation parameters, including pulse width, frequency, amplitude, and pulse train durat
83 imal stimulation settings such as amplitude, pulse-width, frequency and phase for invasive and non-in
84 ed in 3 PD patients simply by increasing the pulse width from 60 to 240 microseconds, even at a lower
85 t 1.55 microm, exhibiting approximately 2 ps pulse width from an Er-doped glass oscillator (ERGO).
86 ales down to 300 ps, comparable to the X-ray pulse width from typical synchrotron sources.
87                        Using tunable voltage pulse widths from 10 us to 100 ms, numerical simulation
88 oth perovskites at 78 K employing short pump pulse width (fs) and near-band gap excitation.
89 uJ high pulse energies and a few nanoseconds pulse width in the near- and mid-infrared regions.
90                       Second, stretching the pulse width in time by introducing negative dispersion w
91                                       As the pulse width increased, the bulk electrical conductivity
92 essful for subsequent ECTs when the 0.5-msec pulse width is used.
93 d discovered that a BP nsEP with symmetrical pulse widths is not required to generate BPC.
94 sent sounds in which the waveform shape, the pulse-width, is fixed throughout the presentation or whe
95                                   A temporal pulse width larger than the time needed for pressure red
96                                        Laser pulse widths less than 1 nsec in the near-IR are capable
97 s generating a temporal resolution below the pulse-width limit.
98  be predominately diffusion rather than gate pulse width limited.
99                                Nearest level pulse width modulation (PWM) is used to generate switchi
100                                    We show a Pulse Width Modulation (PWM) process can periodically ba
101         The mathematical underpinning of the pulse width modulation (PWM) technique lies in the attem
102 l of gene expression using a strategy termed pulse width modulation (PWM).
103 ed in this study, all tested patterns except pulse width modulation, significantly reversed mechanica
104  Tonic (conventional), amplitude modulation, pulse width modulation, sinusoidal rate modulation, and
105 king accuracy by doing away with traditional pulse width modulation; and (iii) a Sliding Mode Control
106 cules over a large concentration range using pulse-width modulation (PWM).
107 om-made actuator arms, in combination with a pulse-width-modulation (PWM) technique, to achieve progr
108  achieved under a duty cycle of <=0.1% and a pulse width of <=2 mus.
109 apture thresholds at 6 months (</=2.0 V at a pulse width of 0.24 msec and an increase of </=1.5 V fro
110                                          The pulse width of 0.5 msec is more efficient than the 1-mse
111 eshold voltage of 4.7 V (2.7-6.7), threshold pulse width of 1.8 ms (1.0-2.5), and an impedance of 120
112 eters: electric field strength of 3kV/cm and pulse width of 10mus after the treatment of 20-h culture
113 atrices recorded for all participants with a pulse width of 25 us and a current level of 110 CL.
114 zation, and a Q-switched pulse output with a pulse width of 5 ns and peak power of 255 W was achieved
115 slope efficiency of 29.4% and with a minimum pulse width of 5.1 ns.
116 t response time is limited only by the laser pulse width of 500 fs, and permits a measurement of the
117 a 1195 MHz signal at 53 dBm peak power and a pulse width of 550 ns at a range of interpulse intervals
118  23.8 mJ of photobleaching light energy at a pulse width of 6 msec and a duty cycle of 50%.
119  of 0.71 J/cm2, repetition rate of 5 Hz, and pulse width of 750 picoseconds in combination with a dif
120 beams in a time shorter than the synchrotron pulse width of about 100 ps.
121 can be changed dynamically by modulating the pulse width of the control signal to a variable focus li
122 uous extraction mode essentially matches the pulse width of the laser (4 ns).
123 tical charge (average mC=2.5 times age) with pulse widths of 0.5 msec and 1 msec and frequencies of 3
124 oF monophasic capacitive-discharge pulses at pulse widths of 1.5, 3.0, 7.5, and 15 ms.
125 hrough this zone is very rapid, resulting in pulse widths of ~200 mus for the nanopores used in this
126 igh frequency and high voltage waveform with pulse widths of ~50 mus (and ~50 mus between pulses) is
127                                            A pulse-width of 100 ms and a pulse-amplitude of 4 mA were
128 nce in response to the varying amplitude and pulse-width of the applied signal.
129  2 mA in achieving spatial entrainment while pulse-widths of 50 ms and 100 ms had comparable effects
130 ars in </=3 ps after 452 nm excitation (5 ps pulse width) of PYP.
131  an absorber, pump laser repetition rate and pulse width on AFM-IR signal amplitudes and spatial reso
132 ngth-duration relationship, or the effect of pulse width on defibrillation efficacy.
133 They also do not include the effect of input pulse width on the output.
134 he relative influence of pulse amplitude and pulse width on the overall effectiveness of stimulation.
135 asurement and quantification of laser power, pulse width optimization, field of view, resolution and
136                            Additionally, the pulse width, p(w), of the pulse flow valve "injection" r
137                                       Paired pulse width pacing thresholds at 2.8 V were compared in
138 acing threshold of up to 2.0 V at a 0.4-msec pulse width (performance goal, 80%).
139 tages declined exponentially with increasing pulse width reaching an asymptote by 6 ms (451+/-68 V, P
140 time-dependent experimental variables (laser pulse width, reagent fluorescence lifetime, etc.).
141    There is a specific optimum voltage, gate pulse width, resolving power, and now CRM for each ion.
142 60 beats per minute, 2 V amplitude, and 1 ms pulse width, restoring mean arterial pressure from 0 to
143 and varied stimulation charge, frequency and pulse width, resulting in over 1000 different potential
144 tage show a strong correlation with positive pulse width, rise and fall time, cycle mean, and area.
145 f some neurons were charge insensitive; (ii) pulse-width sensitivity varied between cell types, allow
146  low current intensity (<5 mA and 100 micros pulse width) stimulation, our results show that all of o
147 uction was more successful with the 0.5-msec pulse width than the 1-msec pulse width.
148 ak heart rates were higher with the 0.5-msec pulse width than the 1-msec pulse width.
149                                      For all pulse widths, the 24-hour MVL-ED50 was lower than the 1-
150 antennas can be reconfigured by the incident pulse width to exhibit directional characteristics varyi
151                        We concomitantly vary pulse width to separate the effect of changing PF on sen
152 learning approach is presented to illustrate pulse-width tunability by replacing part of an existing
153 ntional ion injection mechanisms produce ion pulse widths typically around a few microseconds or less
154 ation by implanted electrodes (10 Hz, 0.3 ms pulse width, up to 6 V, 8 h day-1) for 2 or 7 days with
155 e and time subsequently separate by multiple pulse widths upon free propagation by virtue of their di
156  Compression of optical pulses to ultrashort pulse widths using methods of nonlinear optics is a well
157               The physical limitation of the pulse width was discussed with the calculated results.
158                                      Phase-2 pulse width was held constant at 3 ms in all waveforms.
159 epetitive white light stimulation of varying pulse width was observed.
160 ipolar pacing at an output of 10 mA and 2-ms pulse width was required.
161                                Frequency and pulse width were fixed.
162 perating point, based on frequency-amplitude-pulse width, where a null heart rate response is reprodu
163  found with a higher duty cycle and a longer pulse width, where the antimicrobial efficiency could al
164 osure dose VT (applied voltage x frequency x pulse width x treatment duration) of about 4700 Vs, ther

 
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