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1 icrofluidic chip with a locally amplified AC electric field gradient.
2 d the local density approximation to predict electric field gradients.
3 J and J' states and with them shifts due to electric field gradients.
4 on enrichment and depletion (FIE and FID) on electric field gradients.
6 adient focusing technique that depends on an electric field gradient and a hydrodynamic counterflow t
7 EFGF) is a separation technique that uses an electric field gradient and an opposing hydrodynamic flo
8 contributions to the NMR line shape from the electric field gradient and the anisotropic shielding te
9 oadening arising from the interaction of the electric field gradient and the nuclear electric quadrup
11 produce the Mossbauer parameters (A-tensors, electric field gradient, and isomer shift) of 2 quite we
12 We used COMSOL simulations to calculate the electric field gradients, and these theoretical results
13 posts in a microfluidic device around which electric field gradients are created by the application
14 ing constants, which are proportional to the electric field gradients at the (17)O sites, decrease by
17 ch as in wound healing, and cells respond to electric field gradients by reorienting and migrating di
18 ed to the gold microtubes resulting in large electric field gradients down the length of the tubes.
19 at the charge is partially shielded from the electric field gradient during transport, possibly by th
20 eld splitting was attempted by analyzing the electric field gradient (EFG) at the (57)Fe nuclei, taki
21 nctional theory, the predicted values of the electric field gradient (EFG) or equivalently the C(Q) a
23 ropic chemical shift values and the chlorine electric field gradient (EFG) tensor information are ext
24 ons aimed at predicting the (57)Fe Mossbauer electric field gradient (EFG) tensors (quadrupole splitt
27 c field gradient focusing (DFGF) utilizes an electric field gradient established by a computer-contro
28 We have applied this method in miniaturizing electric field gradient focusing (EFGF) and carrying out
32 l methacrylate-co-methyl methacrylate) micro electric field gradient focusing (muEFGF) device is desc
34 to compute all of the tensor elements of the electric field gradient for each carbon-deuterium bond i
36 ver, an intrinsic by-product of the enormous electric field gradients inherent to plasma accelerators
37 ly associates with the TatBC complex, and an electric field gradient is required for the cargo to pro
38 which describe the formation of an extended electric field gradient leading to concentration enrichm
39 ielectrophoretic force that results from the electric field gradient near the ridges is used to affec
40 te which shows no signature of change in the electric field gradient (nuclear quadrupolar frequency)
41 nt of +/-71.2 +/- 1 MHz, corresponding to an electric field gradient of +/-1.49 atomic units at the c
42 servation that the largest components of the electric field gradients of Fe(O) and Fe(OH) are perpend
44 arbonic anhydrase indicate that the computed electric field gradient tensor is in good agreement with
45 The principal component V(zz) of the (11)B electric field gradient tensor is tilted slightly away (
47 in a comprehensive set of chemical shift and electric field gradient tensors for a small molecular tr
48 pling parameters, and the orientation of the electric field gradient tensors for each site of zinc fo
49 cases, molecular orbital calculations of the electric field gradient tensors yields C(q) and eta valu
50 s demonstrated through the application of an electric field gradient that leads to phase separations
51 PEs can be exploited to shape and extend the electric field gradients that are responsible for DEP fo
53 ymer by Joule heating, extremely non-uniform electric field gradients to polarize and manipulate the
55 omplex electrophoretic setups coupling sharp electric field gradients with bulk reactions, surface re
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