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1 mechanism consistent with a shift in the Ih activation curve.
2 induced a leftward shift of the Ca2+ channel activation curve.
3 his mutation on CaM shifts the KCNQ1 voltage-activation curve.
4 ) amplitude and a depolarizing shift in I(h) activation curve.
5 verns cellular behavior exhibits a sigmoidal activation curve.
6 actions as demonstrated by a shift in PIP(2) activation curve.
7 ve membrane effected a leftward shift in the activation curve.
8 uced a depolarized shift in the steady-state activation curve.
9 fect of mixtures of Ba(2+) and Ca(2+) on the activation curve.
10 a comparable shift in the transducer channel activation curve.
11 induced a negative shift of the steady-state activation curve.
12 d a left shift ( approximately 40 mV) of the activation curve.
13 a significantly more negative and shallower activation curve.
14 ctivation and a hyperpolarizing shift in the activation curve.
15 2 isoform is associated with a more negative activation curve.
16 esulted in a 15 mV depolarizing shift of the activation curve.
17 did not evoke a hyperpolarizing shift in the activation curve.
18 nnels, and induced a negative shift of their activation curves.
19 osition 345 rendered shifted biphasic proton activation curves.
20 proton apparent affinity and biphasic proton activation curves.
21 the nonlinear force versus displacement and activation curves.
22 mutations) or by a depolarizing shift of the activation curve (2 voltage sensor mutations) decreasing
23 ts takes place through shifts in its voltage activation curve, allowing channel opening at physiologi
24 is within the dynamic range of the synaptic activation curve and a shift in the activation curve by
25 mall negative shift in the channel's voltage-activation curve and led to an increased nonselective le
27 le manner but caused a depolarizing shift in activation curves and greater use-dependent block of Ca(
31 ardiac isoform showed a minimal shift in the activation curve as a function of time after whole-cell
33 voltage curves) always preceded the channel activation curves, as expected for protein rearrangement
35 me transport protein based on: (a) different activation curves, (b) different time dependencies, (c)
36 yed or improved exhibit dramatically shifted activation curves because of a change in the rate of cot
37 synaptic activation curve and a shift in the activation curve by the modulatory neuropeptide proctoli
38 hereas a leftward shift in voltage or Ca(2+) activation curves can be observed for P(o) values lower
42 dies, cell permeant cAMP analogs shifted the activation curve for I(H) to depolarized potentials in C
43 d the half-point of the isochronal (7.5 sec) activation curve for IKs by -16 mV at 0.1 microM and -24
44 arizing shift (of approximately 6 mV) in the activation curve for the tetrodotoxin-resistant sodium c
45 ette resulted in a depolarizing shift in the activation curve for the transient channels of approxima
46 ective protein kinase inhibitor, shifted the activation curves for both proximal and distal Na+ chann
47 lated to the overlap of the inactivation and activation curves for I(T)), rhythmogenic properties, no
48 ng single-channel electrophysiology, and the activation curves for wild-type and E71A KcsA are indist
49 a nearly 50 mV shift in the midpoint of the activation curve in a direction consistent with stabiliz
51 late Ih in primary afferents by shifting the activation curve in the depolarizing direction and incre
54 potential to a point on the I(Ca) and I(BK) activation curves in which filtering is optimized like t
56 c current decay is faster, the V(1/2) of the activation curve is shifted in the depolarized direction
57 The bilayer-thickness-dependent shift in the activation curve is suggestive of a decrease in an appar
58 4 expression favored open states by shifting activation curves negative, decreasing the slope of the
61 uced a depolarized shift in the steady-state activation curve of I(A) without altering the inactivati
62 MP-S (an activator of PKA), both shifted the activation curve of Ih to more depolarized potentials an
63 onstants and caused a rightward shift in the activation curve of KCNQ1+minK, but affected none of the
64 , whereas beta1 did not modulate the voltage-activation curve of MSSN, beta1 induced a significant le
66 ase is caused by a depolarizing shift in the activation curve of the native HCN current, which in tur
70 ttributable to a hyperpolarized shift in the activation curve of voltage-gated sodium channels (VGSCs
71 ed comparable leftward shifts in the voltage-activation curves of all three isoforms, indicating that
72 a significant leftward shift of the voltage activation curves of both the MDAL and MANG isoforms.
73 ing to L1042-T1051 alters the profile of the activation curves of full-length and C1-C2 forms of ACV
76 o from 100 to 1 mM did not alter the voltage-activation curve or reversal potential (Vrev) but reduce
77 iated with a 4.4-mV depolarization of the Ih activation curve (P=0.0027) and an increase in mean firi
80 We propose that the steepness of this kinase activation curve simultaneously controls the behavioral
82 d residue (Y75E) causes a right shift of the activation curve ("stiff" phenotype) and abolishes funct
84 process usually produce canonical Boltzmann activation curves that correspond to a simple two-state
85 tion was a result of a leftward shift of the activation curve to higher pH values and a slight shift
86 panied by approximately 30-mmHg shift of the activation curve to lower pressures and slower rates of
89 steps, L283F and T310M caused a shift of the activation curve to more positive potentials and F428S r
90 1 processing and shifted KCNE1/KCNQ1 channel activation curve to more positive potentials in HEK cell
91 Application of internal cAMP shifted the activation curve to more positive potentials, giving a V
94 ated temperature moved Kv11.1a/1b isochronal activation curves to more negative potentials, but shift
95 nal [Ca(2+)] or [Mg(2+)] identically shifted activation curves to the right and identically shifted t
97 to mimic the prepulse effect by shifting the activation curve toward more negative potentials, leavin
98 V1 by shifting the voltage dependence of the activation curves towards more physiological membrane po
100 some cells, the hyperpolarizing shift in the activation curve was accompanied by a decrease in peak c
107 ion-activated currents could be described by activation curves with a half-maximal activation potenti
109 , ICA-069673 induced a negative shift of the activation curves without significantly increasing maxim
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