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1 y, and sometimes interphase pH gradients and electric potentials(-).
2 perimental measurements of excess charge and electric potential.
3 are routinely driven by applying an external electric potential.
4 ng surface leakage current, and altering the electric potential.
5 n electrochemical potentials) instead of the electric potential.
6 anced in the presence of an applied external electric potential.
7 several modes depending on the flow rate and electric potential.
8  focus on the evolution of the extracellular electric potential.
9 electrodes is directed by applying a driving electric potential.
10  reaction triggered by the application of an electric potential.
11  lowered proportionally to the square of the electric potential.
12 ised over a conductive surface at a specific electric potential.
13 pplication of arbitrarily shaped oscillating electric potentials.
14 nly used for iDEP applications under applied electric potentials.
15 s also showed the non-homogeneous intratumor electric potentials.
16 ents, flows of small molecules, and membrane electric potentials.
17 valuate fluxes of ions, as well as resulting electric potentials.
18                                          The electric potential accelerating the aurora-producing ele
19    To study the distribution of the membrane electric potential across the GluR channel pore, we reco
20 y, i.e., the gating effect from the built-in electric potential across the MOF phase junctions enable
21 redox reaction is measured under no external electric potential across the molecule-metal interfaces,
22 ver, extracellular fields feed back onto the electric potential across the neuronal membrane via epha
23                               By maintaining electric potential across upstream segments of the capil
24 u method that applies a series of increasing electric potentials across treatment electrodes and meas
25                                          The electric potential and charge distributions across an el
26   The model yields a full description of the electric potential and charge distributions across the m
27 ver two orders of magnitude by modifying the electric potential and electrode separation.
28                                          The electric potential and fluid velocity are in general obt
29 cal method is first developed to compute the electric potential and local species motion in turns of
30 e interaction between the one-dimensional SL electric potential and the massless Dirac fermions hoste
31 mperature without application of an external electric potential and without irradiation.
32        Despite the magnitude of these upward electric potentials and the expectations from observatio
33 orce for K+ appeared to be the transmembrane electric potential, and in most cases substrate specific
34                                         High electric potential applied to the device induces a tempe
35 lux decrease for the ECPNC membranes with an electric potential applied to their surface was only cau
36  kept at ground and the other channel has no electric potential applied.
37 ategy is presented where direct-current (DC) electric potentials are applied in conjunction with surf
38                                              Electric potentials are applied via two parallel three-d
39 maller internal diameters to which rf and dc electric potentials are co-applied.
40  small internal diameters to which rf and dc electric potentials are coapplied.
41  photons as reagents while also employing an electric potential as a convenient and tunable source or
42  approximately 115 were achieved by applying electric potentials as low as 500 V.
43 anges driven by a harmonic modulation of the electric potential at several dc bias potentials and at
44  affected by the presence and polarity of DC electric potential, being 87-90% lower on the ICE cathod
45            The generation of a transmembrane electric potential by the enzyme upon NADH:Q(1) oxidored
46   Our findings show that the strength of the electric potential can affect the dynamic contact angle
47 in short hydraulic residence times, while an electric potential can be periodically applied to debrom
48  perturbations and local changes in cellular electric potential can stimulate cytoskeletal filaments
49 acidic wash buffer and reverting the applied electric potential, carry-over between samples can be re
50 ng of BaTiO3 polarization results in a large electric potential change in Ge.
51                                        Scalp electric potentials corresponding to the magnetic signal
52 ivate these catalysts by means of a suitable electric potential could pave the way for a true integra
53 e sample solution on application of 300 V dc electric potential, cross the neighboring FLM, and are t
54 1 nm, as the atomically resolved fluctuating electric potential decays very rapidly to a negligible v
55                          To provide the same electric potential (DeltaE(elec)) through the BPEs to co
56 FE catalysts have been mostly focused on the electric potential difference between different surfaces
57 mbrane voltage (Vm), which is defined as the electric potential difference between the cytoplasm and
58 ion is applied to an off-center position, an electric potential difference is built that can drive th
59                               By applying an electric potential difference of 2000 V across the lengt
60 mperature-independent mechanism based on the electric potential difference that builds up along the m
61 ctional flow of electrons in the presence of electric potential difference, has been an important goa
62 table electric current during application of electric potential difference.
63                                              Electric potential differences exist around the vascular
64 aling ions and molecules depend on the local electric potentials, different multicellular potentials
65        Here we report the nanoscale measured electric potential distribution inside operating QCLs by
66 e report the existence of a +0.55 +/- 0.09 V electric potential drop between 250 km and 768 km from a
67 lication of the electric field, a high local electric potential drop is formed across the low ionic s
68 ntial additions of reagents or varying of an electric potential during each cycle to operate(11-16).
69  spectrometer, which was subjected to a high electric potential (e.g., -6 kV).
70 tilized to characterize the distributions of electric potential, electric field, and charges on the m
71 ctly harvesting ambient mechanical energy as electric potential energy through water droplets by maki
72 ptly and significantly alter the surrounding electric potential, exciting the electroluminescence of
73 on and separation experiments across varying electric potentials, flow rates, and TE concentrations.
74    By capacitive coupling the latter creates electric potential fluctuations in a cold chaotic cavity
75 erical methods are employed to determine the electric potential, fluid velocity, and late-time solute
76 ravitational forces, we define the threshold electric potential for particle removal.
77 t pathway can also utilize the transmembrane electric potential for protein transport.
78 t Tat pathway also made use of the thylakoid electric potential for transporting substrates.
79 hermore, the photocycle rate is dependent on electric potential generated by chloride gradients in th
80 ernal to an ICR cell by use of a novel axial electric potential gradient mounted in an external ion a
81            Condensate formation generates an electric potential gradient, which directly affects the
82 rocesses occurring upon the establishment of electric potential gradients, with a wide spectrum of en
83  is applicable to Schrodinger operators with electric potentials growing at infinity.
84 ignificant SOCE required high inner membrane electric potential (>-70 mV) and low resting IP3 concent
85 ediated transduction of magnetic fields into electric potentials has been explored as a means for rem
86 ected to superimposed oscillatory and steady electric potentials, i.e., multimode potentials, that in
87 rient and migrate along the direction of the electric potential in a process known as galvanotaxis.
88             Beside OCP, an external negative electric potential in an electrocatlaytic system was als
89 c waves (SAWs) strongly modulate the shallow electric potential in piezoelectric materials.
90                     The zeta potential is an electric potential in the Debye screening layer of an el
91   Furthermore, it has been found that evoked electric potentials in human cortex are correlated with
92 es made of this material can detect sub-volt electric potentials in salt water.
93 ld-effect transistors (FETs) can also record electric potentials inside cells, and because their perf
94 pair of varactor diodes converts a change in electric potential into a modulation in capacitance, res
95 s are electrochromic, effectively converting electric potentials into optical signals through voltage
96                                  We measured electric potentials intracranially in ten epilepsy patie
97 ive electro-mechanical devices that regulate electric potential, ionic flow, and molecular transport
98 field flow fractionation (EFFF or ElFFF), an electric potential is applied across a narrow gap filled
99 tort the electric field distribution when an electric potential is applied.
100        The conversion of optical power to an electric potential is of general interest for energy app
101                                     However, electric potential is present in all cell types and resu
102 ioning of solution ions generates interphase electric potentials known as Donnan and Nernst potential
103 efficiency elevation, and the alterations in electric potential landscapes in the active devices.
104 rom surface morphology to hydrophobicity and electric potential mapping in both air and liquid, mecha
105  temporal dependencies of charge density and electric potential, matching results obtained from compu
106 bed alizarin-TiO2 coupling under interfacial electric potential may lead to changes in the interfacia
107  metal surfaces and (2) applying low-voltage electric potentials may be used to control Ulva biofouli
108                   During active movement the electric potentials measured from the surface of the mot
109 r the local electric field measured with the electric potential microsensor.
110 eposition is controlled by application of an electric potential of appropriate sign and magnitude bet
111 tyrate concentration signals to the negative electric potential of membranes, widening the nanopores
112  pairs are formed due to the induction of an electric potential of opposite sign in the carbon pore w
113 irectly probe the interphase and interfacial electric potentials of condensates, we have designed and
114  We also infer upward magnetic-field-aligned electric potentials of up to 400 kiloelectronvolts, an o
115 nd reversibly control adhesion using applied electric potentials, offering promise for a variety of a
116       Continuous adsorption under an applied electric potential offers the possibility of nanoscale f
117   Our results demonstrate how an oscillatory electric potential on a catalytic surface may alter anti
118 anating from the cathode is regulated by the electric potential on a grid between the cathode and the
119 investigate here the influence of an applied electric potential on the adsorption of charged polymers
120 sm, that light irradiation reduces the local electric potential on the GOM following a carrier diffus
121  to predict the time-varying distribution of electric potentials on the heart surface based on the el
122 ation occurs without the use of any external electric potential or radiation.
123  any catalyst or application of any external electric potential or radiation.
124 insertion of an electrode, application of an electric potential or the inclusion of a molecular senso
125 to differential diffusion, giving rise to an electric potential Phi in the 100 muV range on the micro
126 membranes primarily by altering the membrane electric potential profile, and the spinning molecular k
127 rom a dataset of high gamma cortical surface electric potentials recorded from human sensorimotor cor
128 hese state-dependent changes in the membrane electric potential reflect a reorientation of the dipole
129  reactions driven by elevated temperature or electric potential remains challenging, largely due to m
130 nts of local surface Ce oxidation states and electric potentials reveal the active ceria regions duri
131 mizing detection sensitivity is aligning the electric potential that triggers the sharpest optical tr
132          We developed a method for achieving electric potential that uses an all-metal geometry based
133 are moved in air by sequentially applying an electric potential to an array of electrodes patterned b
134 rformed to address the effects of an applied electric potential to the adsorption behavior of the red
135  on a metallic nickel surface by applying an electric potential to the AFM tip in the DPN process.
136 adients are created by the application of an electric potential to the extremities of the device.
137 ch can be modulated by the application of an electric potential to the surface during patterning.
138 cess used two polyelectrolytes with opposite electric potentials to control the surface charge of the
139 a trapping model considering a field-aligned electric potential together with the mirror force.
140  photocontrol of transmembrane transport and electric potential using bis(thio)ureas derived from sti
141  and based on condensate-specific interphase electric potentials, we reason that condensates are akin
142 t of constant discrete values of the applied electric potential were acquired for kinetic adsorption
143 ing can be partially reversed by applying an electric potential, which leads to significant changes i
144 tronic tools are rapidly advancing to detect electric potentials within networks of electrogenic cell
145 ctly from the Laplace equation governing the electric potential, without solving either the continuit

 
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