戻る
「早戻しボタン」を押すと検索画面に戻ります。 [閉じる]

コーパス検索結果 (１語後でソート)

通し番号をクリックするとPubMedの該当ページを表示します
1 icrofluidic chip with a locally amplified AC electric field gradient.
2 allic filaments between electrodes along the electric field gradient.
3 on enrichment and depletion (FIE and FID) on electric field gradients.
4 d the local density approximation to predict electric field gradients.
5  J and J' states and with them shifts due to electric field gradients.
6 tructures to generate localized DEP-inducing electric field gradients.
7 cavity photons in regions with strong vacuum electric field gradients.
8                                          The electric-field gradient across the boundary of two solut
9 adient focusing technique that depends on an electric field gradient and a hydrodynamic counterflow t
10 EFGF) is a separation technique that uses an electric field gradient and an opposing hydrodynamic flo
11 contributions to the NMR line shape from the electric field gradient and the anisotropic shielding te
12 oadening arising from the interaction of the electric field gradient and the nuclear electric quadrup
13 ned at the interface due to the strong local electric field gradient and the optimized water orientat
14  Post shapes are contoured easily to control electric field gradients and, hence, DEP behavior.
15 produce the Mossbauer parameters (A-tensors, electric field gradient, and isomer shift) of 2 quite we
16  We used COMSOL simulations to calculate the electric field gradients, and these theoretical results
17  posts in a microfluidic device around which electric field gradients are created by the application
18 81)Br and (127)I) combined with the enhanced electric field gradients around these nuclei existing in
19                     It is concluded that the electric field gradient at the XB donor site is a useful
20 otential across the membrane generates local electric field gradients at pores that activate TRPV1 ch
21 ing constants, which are proportional to the electric field gradients at the (17)O sites, decrease by
22            Electrostatic calculations of the electric field gradients at the vanadium atoms have been
23 buffer ions to pass through and there was no electric field gradient beyond that point.
24 ch as in wound healing, and cells respond to electric field gradients by reorienting and migrating di
25                           We discovered that electric field gradients can be used to control and acce
26 ed to the gold microtubes resulting in large electric field gradients down the length of the tubes.
27 at the charge is partially shielded from the electric field gradient during transport, possibly by th
28 eld splitting was attempted by analyzing the electric field gradient (EFG) at the (57)Fe nuclei, taki
29 nctional theory, the predicted values of the electric field gradient (EFG) or equivalently the C(Q) a
30                  The measured values for the electric field gradient (EFG) or quadrupole coupling con
31 ropic chemical shift values and the chlorine electric field gradient (EFG) tensor information are ext
32  NMR measurements to DFT computations of the electric field gradient (EFG) tensor.
33 ons aimed at predicting the (57)Fe Mossbauer electric field gradient (EFG) tensors (quadrupole splitt
34 T) calculations of (99)Ru chemical shift and electric field gradient (EFG) tensors and their analysis
35                             Calculated (14)N electric field gradients (EFGs) reflect experimentally o
36                                The resulting electric field gradients enable demonstration of a diele
37 c field gradient focusing (DFGF) utilizes an electric field gradient established by a computer-contro
38  quadrupolar mechanism, which is mediated by electric field gradient fluctuations and lacks a detaile
39 We have applied this method in miniaturizing electric field gradient focusing (EFGF) and carrying out
40                   Isotachophoresis (ITP) and electric field gradient focusing (EFGF) are two powerful
41                                              Electric field gradient focusing (EFGF) is a separation
42                                              Electric field gradient focusing (EFGF) is an equilibriu
43 l methacrylate-co-methyl methacrylate) micro electric field gradient focusing (muEFGF) device is desc
44 ns, instead of anions, to be enriched via an electric field gradient focusing mechanism.
45 to compute all of the tensor elements of the electric field gradient for each carbon-deuterium bond i
46 e cars are designed to be stimulated with an electric field gradient from a scanning probe microscopy
47 field potentials (LFPs) to assess the actual electric field gradient imposed by Cb-tDCS in our experi
48                        The isomer shifts and electric field gradients in 1.X exhibit a remarkably str
49 ts of magnetic hyperfine fields and non-zero electric field gradients in Sr(2)IrO(4) have been detect
50 ver, an intrinsic by-product of the enormous electric field gradients inherent to plasma accelerators
51 ly associates with the TatBC complex, and an electric field gradient is required for the cargo to pro
52  which describe the formation of an extended electric field gradient leading to concentration enrichm
53 ielectrophoretic force that results from the electric field gradient near the ridges is used to affec
54 te which shows no signature of change in the electric field gradient (nuclear quadrupolar frequency)
55 nt of +/-71.2 +/- 1 MHz, corresponding to an electric field gradient of +/-1.49 atomic units at the c
56      The ions are guided through an internal electric field gradient of the FmuTP that arises from ch
57 servation that the largest components of the electric field gradients of Fe(O) and Fe(OH) are perpend
58  varying gaps and produces variations of the electric field gradient, provides a versatile tool that
59 uorescence intensity to identify the minimum electric field gradient required to overcome dispersive
60                          To achieve the high electric field gradients required to porate the membrane
61 arbonic anhydrase indicate that the computed electric field gradient tensor is in good agreement with
62   The principal component V(zz) of the (11)B electric field gradient tensor is tilted slightly away (
63  the available experimental data as were the electric field gradient tensor orientations.
64 in a comprehensive set of chemical shift and electric field gradient tensors for a small molecular tr
65 pling parameters, and the orientation of the electric field gradient tensors for each site of zinc fo
66 cases, molecular orbital calculations of the electric field gradient tensors yields C(q) and eta valu
67 s demonstrated through the application of an electric field gradient that leads to phase separations
68 PEs can be exploited to shape and extend the electric field gradients that are responsible for DEP fo
69 conductive polymer that enables the required electric field gradient to be established.
70 ymer by Joule heating, extremely non-uniform electric field gradients to polarize and manipulate the
71                    We achieve an appropriate electric field gradient using a selective ionic focusing
72 ity by controlling the main direction of the electric field gradients using individually driven chann
73                                     A linear electric field gradient was obtained by applying a volta
74                                     Using an electric field gradient, we demonstrated layer-resolved
75 omplex electrophoretic setups coupling sharp electric field gradients with bulk reactions, surface re
76 g of serine indicates an alteration in local electric field gradients within the beta subunit.