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1 ent waveforms, but no impact on the released electric charge.
2 ark changes its flavour without altering its electric charge.
3 rentiates between metabolites based on their electric charge.
4 most famously explaining the quantization of electric charge.
5 ction of DNA hybridization via its intrinsic electric charge.
6 y, low volatility, and possessing a negative electric charge.
7 the atmosphere by taking advantage of their electric charge.
8 after as a potential corollary of quantized electric charge.
9 ell a classic dependence of magnetic flux on electric charge.
10 o fluid flow was impaired by the presence of electric charges.
11 le, stretching the nanofibers and generating electric charges.
12 xample, show that defects direct the flow of electric charges.
13 nsurmountable energetic penalty to burial of electric charges.
14 splay is suppressed since it produces bound electric charges.
15 analogy: Topological zero modes are akin to electric charges.
16 two neighboring polarization fields to avoid electric charges.
17 in the UV range, carrying either one or two electric charges.
19 s seen in numerous eruptions, and groups the electric charges about the plume to form the 'lightning
23 tic mobility, mu(e), is sensitive to the net electric charge and hydrodynamic size of a molecule in s
24 n; spin current is a flux of spin without an electric charge and its transport reflects spin excitati
27 stics, consisting of the bound states of the electric charge and the image magnetic monopole charge.
29 Importantly, a neutron carries spin without electric charge, and therefore it can bring spin into a
30 nner analogous to the way a condenser stores electric charge, and, upon phosphorylation, release a la
33 ertainty, suggesting that for S1 x MgATP the electric charge at the actin binding site is abolished.
35 te value of the product of the net effective electric charges at the actin-myosin interface, /ZMZA/.
36 e modification approach targeted the surface electric charges borne by its additive particles, and wa
37 y topological defects named disclinations to electric charges by associating a charge to a disclinati
38 ow that small molecules with as few as three electric charges can effectively induce attractive inter
40 rasites that become airborne may exploit the electric charge carried by their host to facilitate atta
41 ple hydroxyl groups, nonlinear molecule, and electric charge could physically modify secondary struct
44 rostatic influence on activation mediated by electric charge density on the extracellular and intrace
45 crystals that release up to three times more electric charge density than that produced by PbZr0.52Ti
46 oped a-Si layer contributed to the extracted electric charges due to the suppressed electron-hole rec
47 bbles provided, in addition, new evidence of electric charging during the vapor plume cloud processes
50 trol antibody (MBIso) and MB with a negative electric charge for targeting of leukocytes (MBLc) were
51 ophobic core micelle coupled with a positive electric charge forms an organic complex with DCF that i
53 orrosion rate which, in turn, depends on the electric charge immobilized on the surface of the GaAs/A
55 ed here conclusively demonstrate the role of electric charge in detection sensitivity as well as the
57 ly unfavorable situation of an uncompensated electric charge in the apolar, low-dielectric protein in
58 onstrate experimentally for the diffusion of electric charges in a one-dimensional electrical system
59 ctors may often be described as a process of electric-charge-induced self-assembly, wherein the inter
61 environment, the Coulomb attraction between electric charges is decreased, leading, for example, to
64 nucleotide-dependent changes in cross-bridge electric charge might have in the contractile cycle in m
65 to nanometer scale (1.2-414 nm), volatility, electric charge, morphology, and elemental composition.
69 bundle thickness, which is determined by the electric charge of the filaments, the number of hydropho
71 molecular dynamics simulations suggest that electric charge on graphene can force a DNA homopolymer
72 sual physical properties, such as fractional electric charge or a quantized magnetic field flux, orig
73 tic pulses to control the magnetic flux, the electric charge or the phase difference across a Josephs
76 t of As-Co demonstrated that the quantity of electric charge (Q) decreased with the addition of the i
83 n out of equilibrium by light or the flow of electric charge, the vibrational and electronic degrees
84 on, and electric charge; the pore's size and electric charge; the electric field intensity; and the b
85 ctions of the particle's size, location, and electric charge; the pore's size and electric charge; th
88 in which the flow of spin waves, rather than electric charges, transmits and processes information.
89 adratic energy dependence that result in the electric charge vanishing at high energies, a result kno
90 hown here to exhibit traveling extracellular electric charge when they recover from spatially focused
91 Pyroelectric materials that can generate electric charges when subjected to temperature changes a
94 probes enables measuring the distribution of electric charges, which is encoded in the vector form fa