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1 displayed unique measured FVE radii for each electric field strength.
2 e is critical for increasing the current and electric field strength.
3  programmed based on the distribution of the electric field strength.
4 tes in these steps are minimally affected by electric field strength.
5 e time and directional bias as a function of electric field strength.
6 characteristic dependence of ion mobility on electric field strength.
7  and is found to be nonlinearly dependent on electric field strength.
8 on, as well as with cation concentration and electric field strength.
9 150 ps to many nanoseconds, depending on the electric field strength.
10  dependent on both exosome concentration and electric field strength.
11 ocess is only weakly affected by the applied electric field strength.
12  of rapid buffer exchange and an increase in electric field strength.
13 8-mm separation channel length under 30 V/cm electric field strength.
14 segment, the migration time, and the overall electric field strength.
15 ulled by a gradient force to regions of high electric field strength.
16  may be attained by simple adjustment of the electric field strength.
17 eorganization increased nonlinearly with the electric field strength.
18 ion relating imaging magnification change to electric-field strength.
19 factants are more vulnerable to IRE at lower electric field strengths.
20 f electrochemiluminescence at relatively low electric field strengths.
21  ssDNA at a range of Mg2+ concentrations and electric field strengths.
22 ight separation channel over a wide range of electric field strengths.
23 igned carbon nanotubes (CNTs), under varying electric field strengths.
24 be observed especially when operated at high electric field strengths.
25  varying electrolyte concentrations and weak electric field strengths (0-2 V cm(-1)).
26 ntrol of the cluster orientation at very low electric field strengths (0.18 V mum(-1) ) is achieved.
27 tion does not increase monotonously with the electric field strength above an optimum E(0), which is
28 a Stark shift ruler that enables mapping the electric field strength across the electric double layer
29 r ds-DNA fragments are stronger functions of electric field strength and buffer concentration than th
30             Experimental conditions, such as electric field strength and column temperature, as well
31       Separately, it was found that both the electric field strength and duration of injection affect
32 open segment with concomitant changes of the electric field strength and the flow velocity at the int
33 matography (CEC) have discontinuities of the electric field strength and the flow velocity at the int
34 l cross-sectional area determining the local electric field strength and, thus, the local interaction
35 ore, manipulate, and analyze ions under high electric field strengths and controlled ion-neutral reac
36 coefficients of the DNA at several different electric field strengths and extrapolating the results t
37  The effects of the liquid sheath flow rate, electric field strength, and integration time on sensiti
38             Different solution compositions, electric field strengths, and oscillation frequencies ar
39 s longer surface propagation lengths, higher electric field strengths, and sharper angular resonance
40 d different thermostability depending on the electric field strength applied.
41 eral hundred million volts per centimetre of electric-field strength are required to field-ionize gas
42 ase protein diameter and to E*, the critical electric field strength at which ion emission from dropl
43 his surface-specific method, comparing local electric field strengths at the air-water interface and
44                   After PEF treatment at the electric field strength between 0.2 and 0.5kV/cm, AAO be
45                 Various PEF treatments using electric field strength between 0.2 and 1.2kV/cm and pul
46 by three orders of magnitude as we tuned the electric field strength by a few percent across resonanc
47 We conclude that RH421 detects intramembrane electric field strength changes arising from charge tran
48 s by appropriately adjusting temperature and electric field strength could facilitate their applicati
49 nt primary alcohols characterized at reduced electric field strengths E/N of up to 120 Td with a wate
50 d pressures of 20...60 mbar and high reduced electric field strengths E/N of up to 120 Td.
51 llows operation over a wide range of reduced electric field strengths E/N up to 120 Td, allowing sepa
52 r from the field to the material (for a peak electric field strength exceeding 2.5 volts per angstrom
53 oltage to several volts to induce sufficient electric field strength for efficient bacteria inactivat
54 ical potentials needed to achieve 100's V/cm electric field strengths for rapid electrophoresis.
55 olution was further enhanced by reducing the electric field strength from 200 to 125 V/cm.
56  (DFT) simulations reveal distance-dependent electric field strength from the electrode surface.
57  The MIPEF processing variables studied were electric field strength (from 0.4 to 2.0kV/cm) and numbe
58                                          For electric field strengths >=5 V cm(-1), PEDOT is deposite
59 nce of longitudinal diffusion coefficient on electric field strength has been verified.
60                           An estimate of the electric field strength in the CT state yields approxima
61 oard without amplification, producing modest electric field strengths in the nanochannels (0.2-2 kV/c
62              The EEG changes correlated with electric fields strengths in prefrontal cortices, and no
63                           At relatively high electric field strengths, in a thread where elastic stre
64          Treating fruit mash with a moderate electric field strength increased juice yield and improv
65 llular recording techniques, and the applied electric field strength is continuously updated using a
66 ions of the pulse amplitudes increase as the electric field strength is increased.
67 ening and enhance both the EDL potential and electric field strength, leading to a trigger in the net
68                     Defining E(bo) to be the electric field strength necessary to get rotational resp
69                   At optimal PEF parameters: electric field strength of 3kV/cm and pulse width of 10m
70 rovides the best separation efficiency at an electric field strength of 400 V/cm.
71      The PMMA micro-chip was tested under an electric field strength of 705 V cm-1.
72    Using a separation length of 22 cm and an electric field strength of 750 V/cm, analysis times were
73 -entrant resonant cavity that can achieve an electric field strength of more than 100 kV/m with an in
74 ccur at flow rates of 8 mL/min and less, and electric field strengths of 25 V/cm and greater.
75        Exponential decay pulses with initial electric field strengths of approximately 13.3 kV/cm and
76 s with the monolithic capillaries when using electric field strengths of up to 300 V cm(-1).
77  to characterize the effects of pressure and electric field strength on compensation voltage, ion tra
78  for treating grapes using moderate and high electric field strength on the enhancement of CI and TPI
79 ignificantly related to either the simulated electric field strength or the distance between the IRE
80 roplet size as the key parameter controlling electric field strength, product yield, and selectivity.
81 erences and strongly affected by non-uniform electric field strength profile.
82 he advantage of highly focused and localized electric field strength provided by the micronozzle arra
83  in 3-10 min using broad-range ampholytes at electric field strengths ranging from 25 to 100 V/cm.
84 of IEF were completed in less than 25 min at electric field strengths ranging from 50 to 214 V/cm.
85 tration to width ratios as a function of the electric field strength ratio in the control channels an
86         To address this gap, we measured the electric field strength reaching the bone during noninva
87                               To augment the electric field strength reaching the fracture site durin
88 icacy of noninvasive EBGSs by increasing the electric field strength reaching the fracture site.
89                                    A greater electric field strength renders a more substantial elect
90 ctor-metal homojunction with 50% decrease of electric field strength required in the derivation of st
91 bility of ablating large tumors, because the electric field strength required is often too high to be
92                                   A range of electric field strengths resulting in transient electrop
93 itioned within a nanofunnel at sub-threshold electric field strengths, suggesting the utility of nano
94 ship of the proton transfer barrier with the electric field strength that explains the effectivity of
95                                 Even at high electric field strengths the cell remained largely intac
96 lectrochromatographic parameters such as the electric field strength, the potential drop, and the flo
97 re probed as they electromigrated at varying electric field strength through a crystalline array of s
98 FVE radii were associated with corresponding electric field strengths through the first-order vibrati
99 owing through different outlets to different electric field strength, thus resulting in different imp
100 arious conditions of electrophoresis such as electric field strength, time of electrophoresis, switch
101 eved in approximately 30 min by reducing the electric field strength to 125 V/cm.
102 f variance was used to compare the simulated electric field strength to histologic findings.
103 using immersed electrodes are limited by low electric field strengths to avoid shorting, requiring to
104 ca tubers were treated with PEF at different electric field strengths up to 1.2kV/cm.
105 Square waves applied to the device generated electric field strengths up to 1.3 x 10(5) V/cm at the t
106 osphorus donors in bulk silicon with various electric field strengths up to near avalanche breakdown
107  this offset results from the differences in electric field strength used in the techniques.
108 microfluidic channel and applying a range of electric field strengths, we produce protocells that exh
109                                          The electric field strengths were 200 V/cm for MEKC and 2400
110 stopathologic characteristics, and simulated electric field strengths were assessed.
111                                              Electric field strengths were converted into therapeutic
112                                              Electric field strengths were strongest in superficial b
113 te, built-in sensor for measuring interlayer electric field strengths, which are exceedingly difficul
114 shifted with a magnitude proportional to the electric field strength (with red shifts >1 eV), and in
115 d multiple forms of BSA detected at elevated electric field strengths (with and without urea).
116 ates an ionic current with a greatly reduced electric field strength, with particular benefits for li

 
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