ライフサイエンスコーパス: dipole

1 action between the active site and the helix dipole.

2 d that the cage shields around 75% of the HF dipole.

3 ferred, despite repulsion from the push-pull dipole.

4 ative effect of the *C-O to the incoming 1,3-dipole.

5 her than with the spatial summation of local dipoles.

6 n interaction of charges with methylammonium dipoles.

7 ge-current configurations involving toroidal dipoles.

8 ivity, instead of the electron-pinned defect-dipoles.

9 ion, distinct from the magnetic and electric dipoles.

10 the atoms as coherent, interacting radiating dipoles.

11 contributions from state filling and surface dipoles.

12 ctive recognition sites, or even charges and dipoles.

13 that have fast rates of reactivity with 1,3-dipoles.

14 esemble, strikingly, Ve generated by current dipoles.

15 for each network, and propose a simple point dipole 2D lattice model that successfully explains the e

16 ltrafast orientational disorder of molecular dipoles, activated at approximately 165 K, acts as an ad

17 find electromagnon excitations and electric dipole active two-magnon excitations in the magnetically

18 aining polar molecules having their electric dipoles aligned parallel to such surfaces.

19 lected because its energetics and transition dipole alignment uniquely allow for the unambiguous iden

20 -handle external techniques for managing the dipoles' alignment.

21 Second, a polarized transition optical dipole allows us to assign the 1.3 ps time constant to t

22 water due to molecular ordering), orienting dipole along the electric field and efficient electrical

23 cale, so that their activity involves torque dipoles alongside the force dipoles usually considered.

24 that these contacts include catalytic charge-dipole and CH-pi interactions that preferentially stabil

25 e enhance our theory to accurately reproduce dipole and non-dipole features of Ve responses to monaur

26 transmission minima are associated with the dipole and quadrupole modes of the cross, the frequencie

27 he presence of a triple bond in both the 1,3-dipole and the dipolarophile and additionally an aryl su

28 se of the weak coupling between the magnetic dipole and the electromagnetic field.

29 ) from combined polarization of CF interface dipoles and electrical-double-layer formation.

30 onfinement and the orientation of electronic dipoles and fields.

31 ical activity in which the sense of electric dipoles and magnetic dipoles become uncoupled when elect

32 e nanoscale, the interaction between the dye dipoles and surface plasmons can be finely tuned by coup

33 leading and trailing cells form contractile dipoles and synchronize the formation of new frontal TAs

34 to an anesthetic's hydrophobicity, permanent dipole, and polarizability, and is accepted to occur in

35 ee lowest-order multipoles-the total charge, dipole, and quadrupole moment-we show that the value of

36 key climate modes (El Nino, the Indian Ocean dipole, and the southern annular mode).

37 models of fibrous matrix, cytoskeletal force dipoles, and the lamin A gene circuit illustrate the wid

38 Indian Ocean, where physically coherent SST dipole anomalies appear to form a necessary condition fo

39 shes for centrosymmetric materials under the dipole approximation.

40 bining both comprehensive numerical discrete dipole approximations (DDA) simulation and transmission

41 The dipoles arising from adsorbed counterions on polymer bac

42 a pair of opposite charges and the magnetic dipole as a current loop, the toroidal dipole correspond

43 bonding (F...HN) and N(+)...F(delta-) charge-dipole attraction compel the amide carbonyl groups to or

44 distance between the origin and location of dipole band at 20 dB attenuation, indicating that they h

45 With the implementation of dipole band model and abdomen model, the performances of

46 h the sense of electric dipoles and magnetic dipoles become uncoupled when electrons can circulate ar

47 The collective dipole behaviors in (BaTiO3)m/(SrTiO3)n composite nanowi

48 The active 1,3 dipole benzothiazolium N-phenacylide was generated in si

49 opean region, the data also imply a climatic dipole between Europe and East Asia since the cold-warm

50 suggest that DHA and the channel form an ion-dipole bond to promote opening and demonstrate the chann

51 stems as having closed shell, charge-induced dipole bonding.

52 ndicating the partial shielding of the water dipole by the encapsulating cage.

53 roscopy, and prove the existence of vertical dipoles by second harmonic generation and piezoresponse

54 lifetime measurement and interacting lattice-dipole calculation reveal that the metal-mediated dipole

55 While the electric dipole can be understood as a pair of opposite charges a

56 crust is orders of magnitude larger than the dipole component inferred from spin-down measurements.

57 Strong El-Nino and positive Indian Ocean Dipole conditions are associated with an increase in the

58 The dipole configuration of the Earth's magnetic field allow

59 netic dipole as a current loop, the toroidal dipole corresponds to currents flowing on the surface of

60 the free layer e.g., utilizing the magnetic dipole coupling between them can circumvent this issue.

61 r additional factors including AuNC magnetic dipoles, density of excited-states, dephasing time, and

62 The singularity in the dipole-dipole coupling, referred to as a super-Coulombic

63 Identified as Li bond, the strong dipole-dipole interaction between Li polysulfides and Li

64 n explicit solvent strongly suggest that the dipole-dipole interaction between the carbonate groups i

65 attribute this result to the strong dynamic dipole-dipole interaction between the two vortex cores,

66 e calculation reveal that the metal-mediated dipole-dipole interaction shortens the fluorescent lifet

67 in a circular nanomagnet by manipulating its dipole-dipole interaction with another vortex core confi

68 -qubit gates exploit a second-order electric dipole-dipole interaction, allowing selective coupling b

69 rt electrostatics, in the form of orthogonal dipole-dipole interaction, as the main driver for this a

70 ms are predominantly coupled by the magnetic dipole-dipole interaction, which, according to our obser

71 ng mechanism was verified to be the electric dipole-dipole interaction.

72 B effects outweigh those of hybridization or dipole-dipole interaction.

73 3 at a distance of 8 nm, within the range of dipole-dipole interaction.

74 d to ion-ion interactions (salt bridges) and dipole-dipole interactions (hydrogen bonds), but neverth

75 ondon forces based on pair-wise summation of dipole-dipole interactions across an interface or a gap

76 agnetic fields' abilities to induce magnetic dipole-dipole interactions or control the orientation of

77 dicating the presence of coherent long-range dipole-dipole interactions, as in ice.

78 uid crystal monomer (LCM) system with strong dipole-dipole interactions, resulting in a stable nemati

79 Dipole-dipole interactions, which govern phenomena such

80 atic interactions and O(delta-) ...H(delta+) dipole-dipole interactions, while the guest-guest intera

81 specific (i.e., H-bonding) and nonspecific (dipole-dipole, dipole-induced and instantaneous dipole i

82 This introduces the new chemical concept of "dipole-discriminating electrophilic anions."

83 -fluorosydnones, a unique class of mesoionic dipoles displaying exquisite reactivity towards both cop

84 Dipole distortion energies are responsible for approxima

85 These image-dipole effects are generally not taken into account in s

86 e membrane (bending rigidity and surface and dipole electrostatic potentials) and the susceptibility

87 Each luminescence image was fit to a three-dipole emission model to generate fit residuals that vis

88 use an artificial atom with a large optical dipole enabling 100-fold improvement of the photon detec

89 oinhibition by precluding a highly conserved dipole-enhanced hydrogen bond between the phosphodiester

90 We show that the dipole-exchange spin waves excited in this system have a

91 perimental observations of resonant toroidal dipole excitations in metamaterials and the discovery of

92 heory to accurately reproduce dipole and non-dipole features of Ve responses to monaural tones with f

93 ing northwest, contributing to growth of the dipole field.

94 Emission from a dipole forbidden intermediate state may even dominate th

95 d-d transitions arising from hole doping are dipole forbidden.

96 It is shown that dipole forces strongly respond to polarized light in con

97 subsequent tandem cascade sequence involving dipole formation/cycloaddition in either an intra- or in

98 rimentally investigated frustrated arrays of dipoles forming two-dimensional artificial spin ices wit

99 globe strongly support the geocentric axial dipole (GAD) hypothesis for the past few million years.

100 The densely packed C-F surface dipoles generate a short-range electric field that decay

101 es, N-acyl iminium salts, and ultimately 1,3-dipoles, i.e., Munchnones, for subsequent cycloaddition.

102 y demonstrating that prFMN can function as a dipole in a 1,3 dipolar cyclo-addition reaction as the i

103 A toroidal dipole in metasurfaces provides an alternate approach fo

104 The normal component of the molecular dipole in the SAM, toward or away from the underlying su

105 While the presence of permanent dipoles in aqueous suspensions has been previously sugge

106 MMN source analysis indicated dipoles in both auditory cortex and anterior insula, whe

107 irect experiments, the presence of permanent dipoles in commonly used spherical poly(methyl methacryl

108 ar electrostatic repulsions and forces local dipoles in each layer of the stacked strands to align in

109 The possible quantum liquids of electric dipoles in frustrated dielectrics open up a fresh playgr

110 same as the microscopic chirality of torque dipoles in one regime, the two are opposite in another.

111 an optimum relative orientation between the dipoles in the donor (i.e., InGaN/GaN MQWs) and the dipl

112 ess from the unfavorable orientation of bond dipoles in the equatorial conformer, a destabilizing ele

113 teroatoms increase the reactivity of the 1,3-dipoles in the order of O > NH congruent with S, whereas

114 her analysing the observed data, we define a dipole index of the SSSA between the central equatorial

115 Compared with previous SSSA dipole indices, this index has advantages in detecting t

116 ole-dipole, dipole-induced and instantaneous dipole induced forces) intermolecular interactions are e

117 tive analytical model analysis suggest local dipole induced Rashba effect (R-2) with spin-layer locki

118 nts these nanorods from spontaneous magnetic-dipole-induced aggregation, while their magnetic anisotr

119 , H-bonding) and nonspecific (dipole-dipole, dipole-induced and instantaneous dipole induced forces)

120 ovides a useful measure for correcting image-dipole-induced distortions.

121 cts including Purcell enhancement (F=42) and dipole-induced transparency are observed on the highly c

122 strong and coherent interaction between the dipoles inside the 2DMA dominates its fluorescent decay

123 We find that in addition to ligand dipole, inter-QD ligand shell inter-digitization contrib

124 ast to conventional multipoles, the toroidal dipole interaction strength depends on the time derivati

125 he inhibitory helix requires a buried charge-dipole interaction with helix H1 of the ETS domain.

126 design of this self-healing polymer uses ion-dipole interactions as the dynamic motif.

127 1000-fold enhancement in affinity due to ion-dipole interactions at the second ureidyl C horizontal l

128 ts underscore the significance of long-range dipole interactions in dense OCS, leading to an extended

129 ,6''-positions, which provided ancillary ion-dipole interactions in the coordination process and extr

130 ions, and theoretical modeling of collective dipole interactions in tubulin to investigate the effect

131 deff = 4 + z due to the effect of long-range dipole interactions in uniaxial as opposed to multiaxial

132 nyl represents an interesting example of ion-dipole interactions that has so far received little atte

133 entation induced by multiple terahertz field-dipole interactions.

134 ized by a combination of hydrophobic and ion-dipole interactions.

135 include van der Waals, hydrogen bonding, and dipole interactions; side-chain conformational entropy;

136 sociated constructive/destructive transition-dipole interference that results in intense (epsilon app

137 ropical Indian Ocean during the Indian Ocean Dipole (IOD), an index describing the dipole variability

138 The toroidal dipole is a localized electromagnetic excitation, distin

139 a specific orientation, where the antibiotic dipole is aligned along the electric field inside the po

140 The radiated power from toroidal dipole is also compared with that from conventional elec

141 Finally, the mechanism of the SSSA dipole is investigated by dynamical diagnosis.

142 lts by others that the Sun's electromagnetic dipole is moving toward the Sun's Equator during a solar

143 emblies, shows that the effectiveness of the dipole is similar to that in RS-1.

144 that the expectation value of the permanent dipole is, to lowest order, proportional to the product

145 activity between differently substituted 1,3-dipoles is driven by distortion, whereas the difference

146 Inducing and controlling electric dipoles is hindered in the ultrathin limit by the finite

147 A characteristic feature of toroidal dipoles is tightly confined loops of oscillating magneti

148 he N...N axis, which reorients the molecular dipole, is the dominant motion in all phases, with an ac

149 driven by the formation of a near-spherical dipole layer shell structure around the anion.

150 zoline) (PEOz) can be successfully used as a dipole layer.

151 eting inhibition (the latter contributes non-dipole-like features to Ve responses).

152 s when operating in the near-field region of dipole-like sources.

153 O), that accounts qualitatively for observed dipole-like Ve patterns in sustained responses to monaur

154 romising candidate for the proposed electric-dipole liquid.

155 Here we propose that quantum electric-dipole liquids, analogues of quantum spin liquids, could

156 ngth, with a long-term average virtual axial dipole magnetic moment of the Earth of only 4.9 +/- 2.4

157 this observation is grounded in the electric dipole-magnetic dipole polarizability contribution to op

158 Here, we exploit the different dipole magnitudes and orientations of carboranethiol and

159 er than could be realized with the loops and dipoles, making the microscopic RF in-vivo transmitting

160 ons between macroscopically separated atomic dipoles mediated by an optical waveguide.

161 influence over molecular conformation due to dipole minimization effects.

162 tion (ENSO), the Atlantic Nio and the Indian Dipole Mode.

163 e a useful alternative to equivalent-current dipole models in localisation of auditory evoked respons

164 mformer performed equally well as the single-dipole models in terms of accuracy for both the N1m and

165 ng charge, Drude oscillator, and the induced dipole models), the angular overlap model, and valence b

166 e also compared with more traditional single-dipole models.

167 quartz substrates, the electric and magnetic dipole modes are easily identifiable across a wide range

168 dex Silicon substrates, even the fundamental dipole modes do not have a clear association.

169 (2DMA), a thin sheet of strongly interacting dipole molecules self-assembled at close distance on an

170 geomagnetic spike" [defined as virtual axial dipole moment > 160 ZAm(2) (10(21) Am(2))] is further co

171 W-DF, Vydrov-Van Voorhis (VV), exchange-hole dipole moment (XDM), Tkatchenko-Scheffler (TS), many-bod

172 24, 36, 48 and 60h) and solvent polarities (dipole moment - hexane: 0.0, diethyl ether: 2.80, ethyl

173 Dipole moment also correlates with isomer toxicity.

174 ositively with the strength of the molecular dipole moment and it is reduced with increasing molecula

175 ose states because of their small transition dipole moment and overlap with the B850/B870 exciton ban

176 bstituent, the isomer having both the higher dipole moment and the electron-withdrawing group in the

177 physicochemical parameters demonstrates that dipole moment and the lowest unoccupied molecular orbita

178 vity, (iii) cell-wall's electronegativity or dipole moment and their relaxation and (iv) charge carri

179 tion to possibly having a permanent electric dipole moment as a consequence of violation of time-reve

180 The dipole moment calculated for the heaxafluorocyclohexane

181 a manifold of close-lying excited states and dipole moment changes between ground and excited states

182 orrelated with the component of the electric dipole moment in the aromatic ring, suggesting that an a

183 sal invariance, develops an induced electric dipole moment in the presence of an external electric fi

184 above 5 D, whereas in 2b and 2d ground state dipole moment is significantly reduced.

185 tric constant is consistent with an electric dipole moment of 0.51+/-0.05 Debye for an encapsulated w

186 The dipole moment of HF@C60 was estimated from the temperatu

187 charge, rotational diffusion coefficient and dipole moment of individual proteins.

188 Our simulations show that the electric dipole moment of residues around heme a changes with the

189 ng the variable bond length with their giant dipole moment of several hundred Debye, we observe count

190 In the dyad, the electronic transition dipole moment of the electron donor perylene is aligned

191 rection resulting from hydrogen bonding, the dipole moment of the ion-pair transition state is an imp

192 tially complicated by the large ground state dipole moment of the nitrile, which may irrevocably pert

193 A strong permanent dipole moment on the sulfobetaine moiety was calculated

194 ription of these two phenomena, in which the dipole moment operator, [Formula: see text], is not cons

195 eir latent heat of evaporation and molecular dipole moment over a wide concentration range with sub-p

196 gnetic moment mu at a site of local electric dipole moment p, it is unknown to date whether mu prefer

197 erized by a quantized and unbounded magnetic dipole moment parallel to their propagation direction.

198 T, where the direction of the ThT transition dipole moment S(0) --> S(1)* is not changed either by th

199 any-body representation of the potential and dipole moment surfaces and VSCF/VCI calculations of vibr

200 ate, which cancels out its overall molecular dipole moment to facilitate charge transport.

201 he resultant orientation of their transition dipole moment vectors was measured by angle-dependent p-

202 on can be affected by the permanent electric dipole moment which could be adjusted by modifying the c

203 s show that the interaction of the P1 domain dipole moment with the TM electrical field considerably

204 he direction(s) of the absorption transition dipole moment(s) (TDMs) in the molecular frame of refere

205 in past and future searches for a permanent dipole moment, and show that the neutron electric polari

206 iffusion coefficient, coordinate number, and dipole moment, as well as the infrared and Raman spectra

207 arge localization, and thus the ground-state dipole moment, consistent with the contracted antiparall

208 he column orientation, and thus the columnar dipole moment, is receptive to geometric frustration if

209 transitions with a zero in-plane transition dipole moment, making their detection with conventional

210 incides with the direction of the transition dipole moment, or by the rotation of the ThT molecule as

211 nding energy and its fundamental components, dipole moment, polarizability, and orbital energies, can

212 tip to the dark exciton out-of-plane optical dipole moment, with a large Purcell factor of >/=2 x 10(

213 relativity or searches for electron electric dipole moment.

214 ead to an increase of its permanent electric dipole moment.

215 ility and the time-averaged dynamic electric dipole moment.

216 er from in terms of density distribution and dipole moment.

217 rface hydrophobicity, and (iii) the electric dipole moment.

218 Permanent electric dipole moments are important for understanding symmetry

219 res of polar, water tetramer clusters having dipole moments between 2D and 3D.

220 The difference dipole moments for these states show that electron densi

221 t the angular distribution of the transition dipole moments is bimodal.

222 electively enhances optical transitions with dipole moments normal to the two-dimensional plane, enab

223 ma, where alignment of electric and magnetic dipole moments occurs.

224 Instead, the large, approximately 3.6 D dipole moments of the histidine side chains effectively

225 re mechanisms because of the large permanent dipole moments of the two reactants.

226 elling the net orientation of the transition dipole moments of these materials yields general design

227 gnetic colloidal nanoplates order with their dipole moments parallel to each other but pointing at an

228 ly different quantum mechanically calculated dipole moments, a factor that can be further exploited t

229 stribution of compositions, surface charges, dipole moments, modular and combined functionalities, wh

230 oltz plane and adsorbed species having large dipole moments.

231 is demonstrated by moderately large nonzero dipole moments.

232 enerates a cyclohexane with a high molecular dipole (mu = 6.2 D), unusual in an otherwise aliphatic c

233 monoxide and alkyne-tethered imines into 1,3-dipoles (Munchnones), which undergo spontaneous, intramo

234 trate that the coupling between the magnetic dipole of a spin and the electromagnetic field can be en

235 the structure, degree of order, and internal dipole of each molecule.

236 ronic rather than steric arguments, with the dipole of the acceptor substituent flanking the carbene

237 Different 1,3-dipoles of allenyl-type were employed, giving different

238 dimension induces net electric and magnetic dipoles of split-ring resonators parallel or anti-parall

239 heq conformer by repulsion of unidirectional dipoles of the endocyclic oxygen lone pair and of the hi

240 riven by interactions between the transition dipoles of the ligands, and subsequently into geometrica

241 e electric field generated by loosely packed dipoles on mixed F/H-terminated surfaces has a considera

242 hat such nanowire systems exhibit intriguing dipole orders, due to the combining effect of the anisot

243 The dipole orientation can be reversed by a critical electri

244 The competition between shape anisotropy and dipole orientation generates mesoscopic isomerism.

245 r nonlinear signals resulting from molecular dipole orientation induced by multiple terahertz field-d

246 differences in detergent headgroup charge or dipole orientation.

247 ays new spectral features whose energies and dipole orientations are consistent with dark neutral and

248 nfinement at base, which induces a permanent dipole oriented from base to apex.

249 that these gases alter collective terahertz dipole oscillations in a manner that is correlated with

250 polar metal that exhibits long-range ordered dipoles owing to cooperative atomic displacements aligne

251 ecise knowledge about the shapes, growth and dipole patterns of polar nanoregions has led to the char

252 by both variation of the intensity-dependent dipole phase as well as finite spatial coherence of the

253 that expected from the noninteracting single-dipole picture.

254 the emission and the far field radiation for dipoles placed in the gap between a metallic nanorod, or

255 is grounded in the electric dipole-magnetic dipole polarizability contribution to optical activity i

256 process in a Bosonic quantum gas, an optical-dipole potential arising from the internally-generated f

257 the dependence of conformational kinetics on dipole potential modifiers.

258 packing density cause changes in local lipid dipole potential that are responsible for the dependence

259 Toroidal dipoles provide physically significant contributions to

260 This SSSA dipole provides a positive feedback to the formation of

261 ave symmetries resembling that of monopoles, dipoles, quadrupoles and octupoles corresponding to fill

262 the ensuing bonding inaccessible to elastic dipoles, quadrupoles and other nematic colloids studied

263 ta the orientation of GFP and its transition dipole relative to the integrin head, and measure orient

264 ation of the lowest-lying MLCT excited state dipole relative to the ligand that contained the carboxy

265 d to approximately 110 meV for the analogous dipole reorientation of MA.

266 ational model incorporating line tension and dipole repulsion indicated that even small changes in li

267 where antiferroelectrically coupled electric dipoles reside on a triangular lattice.

268 nce modulation of up to 0.35 at the magnetic dipole resonance of the metasurfaces and a spectral shif

269 ctive interference of electric- and magnetic-dipole responses of nanoparticle array with the wave ref

270 rk due to the degeneracy of the ground-state dipole rotational energy barrier of the system.

271 fined spheroids of sub-10 nm size with local dipoles self-aligned in a direction opposite to the macr

272 el describing bacteria as hydrodynamic force dipoles shows that steric effects, hydrodynamics interac

273 , this index has advantages in detecting the dipole signals and in characterizing their relationship

274 io-frequency deflector in combination with a dipole spectrometer not only allows for single-shot extr

275 The cytoplasmic site nucleates headgroup-dipole stacking interactions that form a chain of lipid

276 e nanowires, with the appearance of fruitful dipole states (including those being purely polar, purel

277 eriod from 1982 to 2014, from which the SSSA dipole structure is identified for boreal autumn.

278 An emitter near a surface induces an image dipole that can modify the observed emission intensity a

279 e alkali halide layer, inducing out-of-plane dipoles that are stabilized in one orientation (self-pol

280 e carriers within a metal eliminate internal dipoles that may arise owing to asymmetric charge distri

281 nt properties, i.e., the Pt NP-metal surface dipole, the Coulomb blockade and quantum confinement eff

282 Employing vinyl isocyanates as 1,4-dipoles, the cycloannulation occurs under relatively mil

283 uring regions of oppositely aligned magnetic dipoles, their equivalent in optics have not been fully

284 reshwater reproduce the initial hydroclimate dipole through sea-ice feedbacks in the Nordic Seas.

285 ave been affected by a micron-scale magnetic dipole, thus establishing that our sorter can be an inst

286 We attribute this wet-dry dipole to the location of the maximum sea surface warmin

287 whereas 1,3-dipolar cycloadditions of these dipoles to typical acetylenic and olefinic dipolarophile

288 a superposition of two lowest states without dipole transition between them.

289 Within each dipole type, the predicted cycloaddition reactivities co

290 ht-matter interactions through a plethora of dipole-type polaritonic excitations have been observed i

291 involves torque dipoles alongside the force dipoles usually considered.

292 Ocean Dipole (IOD), an index describing the dipole variability of the SSSA has been pursued recently

293 o the sea surface temperature anomaly (SSTA) dipole variability.

294 ound to have a largely horizontal transition dipole vector orientation relative to the substrate, whe

295 around the fictitious arrow of the toroidal dipole vector.

296 Stabilities of the dipoles were assessed by various homodesmotic schemes an

297 to field-induced alignment of the molecular dipoles, which reduces the vibrational freedom of the la

298 omenon originates from the effect of surface dipoles, which together with the weak Fermi level pinnin

299 ) consist of randomly distributed dot pairs (dipoles) whose orientations are determined by specific g

300 y represents 2008 as a negative Indian Ocean Dipole year.