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1 anced in the presence of an applied external electric potential.
2 several modes depending on the flow rate and electric potential.
3 focus on the evolution of the extracellular electric potential.
4 electrodes is directed by applying a driving electric potential.
5 reaction triggered by the application of an electric potential.
6 pplication of arbitrarily shaped oscillating electric potentials.
7 nly used for iDEP applications under applied electric potentials.
8 ents, flows of small molecules, and membrane electric potentials.
9 valuate fluxes of ions, as well as resulting electric potentials.
10 To study the distribution of the membrane electric potential across the GluR channel pore, we reco
11 redox reaction is measured under no external electric potential across the molecule-metal interfaces,
12 ver, extracellular fields feed back onto the electric potential across the neuronal membrane via epha
15 cal method is first developed to compute the electric potential and local species motion in turns of
17 orce for K+ appeared to be the transmembrane electric potential, and in most cases substrate specific
19 lux decrease for the ECPNC membranes with an electric potential applied to their surface was only cau
24 anges driven by a harmonic modulation of the electric potential at several dc bias potentials and at
25 affected by the presence and polarity of DC electric potential, being 87-90% lower on the ICE cathod
27 acidic wash buffer and reverting the applied electric potential, carry-over between samples can be re
29 e sample solution on application of 300 V dc electric potential, cross the neighboring FLM, and are t
30 ctional flow of electrons in the presence of electric potential difference, has been an important goa
33 lication of the electric field, a high local electric potential drop is formed across the low ionic s
34 tilized to characterize the distributions of electric potential, electric field, and charges on the m
35 ctly harvesting ambient mechanical energy as electric potential energy through water droplets by maki
36 ptly and significantly alter the surrounding electric potential, exciting the electroluminescence of
37 By capacitive coupling the latter creates electric potential fluctuations in a cold chaotic cavity
38 erical methods are employed to determine the electric potential, fluid velocity, and late-time solute
41 hermore, the photocycle rate is dependent on electric potential generated by chloride gradients in th
42 ernal to an ICR cell by use of a novel axial electric potential gradient mounted in an external ion a
44 ignificant SOCE required high inner membrane electric potential (>-70 mV) and low resting IP3 concent
45 rient and migrate along the direction of the electric potential in a process known as galvanotaxis.
47 Furthermore, it has been found that evoked electric potentials in human cortex are correlated with
49 ld-effect transistors (FETs) can also record electric potentials inside cells, and because their perf
51 ive electro-mechanical devices that regulate electric potential, ionic flow, and molecular transport
52 field flow fractionation (EFFF or ElFFF), an electric potential is applied across a narrow gap filled
55 bed alizarin-TiO2 coupling under interfacial electric potential may lead to changes in the interfacia
57 eposition is controlled by application of an electric potential of appropriate sign and magnitude bet
58 pairs are formed due to the induction of an electric potential of opposite sign in the carbon pore w
59 We also infer upward magnetic-field-aligned electric potentials of up to 400 kiloelectronvolts, an o
61 anating from the cathode is regulated by the electric potential on a grid between the cathode and the
62 investigate here the influence of an applied electric potential on the adsorption of charged polymers
63 to predict the time-varying distribution of electric potentials on the heart surface based on the el
64 insertion of an electrode, application of an electric potential or the inclusion of a molecular senso
65 to differential diffusion, giving rise to an electric potential Phi in the 100 muV range on the micro
66 membranes primarily by altering the membrane electric potential profile, and the spinning molecular k
67 hese state-dependent changes in the membrane electric potential reflect a reorientation of the dipole
68 nts of local surface Ce oxidation states and electric potentials reveal the active ceria regions duri
70 are moved in air by sequentially applying an electric potential to an array of electrodes patterned b
71 on a metallic nickel surface by applying an electric potential to the AFM tip in the DPN process.
72 adients are created by the application of an electric potential to the extremities of the device.
73 ch can be modulated by the application of an electric potential to the surface during patterning.
74 cess used two polyelectrolytes with opposite electric potentials to control the surface charge of the
75 ing can be partially reversed by applying an electric potential, which leads to significant changes i
76 ctly from the Laplace equation governing the electric potential, without solving either the continuit
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