ライフサイエンスコーパス: dipole

1 ure variability including the North American Dipole.

2 valuable precursor of the nitrile imine 1,3-dipole.

3 across continental scales, known as climate dipoles.

4 cations that arises from frustrated electric dipoles.

5 generates molecular distortions and electric dipoles.

6 rly independent and quasi-classical magnetic dipoles.

7 etric linkers supporting oriented electronic dipoles.

8 noscale domain boundaries of locally ordered dipoles.

9 labels through interactions with their macro-dipoles.

10 ce their cycloaddition rates with Type I-III dipoles.

11 roelectric) collinear alignments of electric dipoles.

12 tributed to the interfacial coupling between dipoles across the filler/polymer interfaces.

13 We find that extensile force dipole activity stabilizes complex defect configurations

14 acids orient around 94% of the nearest water dipoles against the protein surface, and the correlation

15 The capability to modulate dipole alignment by varying gas pressure at constant nor

16 Analysis of the dynamic evolution of dipole alignment in the simulations reveals that, while,

17 by density functional theory calculations of dipole-allowed transitions in Fe:MoS(2).

18 with the positive phase of the Indian Ocean Dipole, although the positive PMM phase and El Nino Modo

19 This suggests that dipole and band-edge engineering must be a primary desig

20 isite starting materials, method definition, dipole and dipolarophile scope, ten-fold scale-up reacti

21 HG nonlinearity majorly result from magnetic dipole and electric quadrupole clearly provides potentia

22 The nuclear magnetic dipole and nuclear electric quadrupole hyperfine structu

23 ubic structure to an incommensurate electric dipole and orbital helix via an intermediate density wav

24 structures of lemon, star, monstar, spiral, dipole and quadrupole are created by the superpositions

25 versions of flexible, screen printed folded dipoles and a meandered monopole operating in the 915 MH

26 h the selective DOC of SASFs with a range of dipoles and cyclic dienes, we report a diverse click-lib

27 ay a very characteristic pattern of trailing dipoles and prismatic loops which are absent in uncharge

28 riply forbidden by the electric and magnetic dipoles and the electric quadrupole.

29 The facility to derivatize these dipoles and to tune their reactivity toward cycloadditio

30 nic symmetry (as defined by large transition dipoles) and then assembled them into MOFs.

31 , nitrile oxides, diazo compounds, and other dipoles), and [4 + 2] cycloadditions (mainly Diels-Alder

32 properties by modifying the strength of the dipole, and (ii) an increase in the viscosity of the sol

33 level alignment, the importance of interface dipoles, and band bending as the result of interface for

34 ve intermediates with activated olefins, 1,3-dipoles, and dienes, the process generates diverse molec

35 aracterized by their stabilization energies, dipoles, and Maximally-Localized Wannier Function (MLWF)

36 the internal oscillatory current to drive a dipole antenna, which radiates into free space.

37 he cooperative mode line shifts of the point dipole approximation begin to rapidly diverge at small s

38 l features arising from the breakdown of the dipole approximation for the emission.

39 om and the mode wavelength is increased, the dipole approximation no longer holds and the atom is ref

40 quantum electrodynamics typically invoke the dipole approximation(1,2), in which atoms are treated as

41 e a detailed study for the validity of point dipole approximations in small systems of strongly coupl

42 describe such systems have resulted in point-dipole approximations to resonators that are computation

43 study systems of magnetic dipoles where the dipoles are arranged on various types of one-dimensional

44 tmospheric processes, climate and ecological dipoles are likely to shift in their intensity, distribu

45 field-driven reorientation of the individual dipole, as the coercive field provides the necessary ene

46 damentally smallest emitters of light, i.e., dipoles, as an indicator.

47 silver electrode due to the proximity of the dipole associated with the amide (or related) group, and

48 ng between the induced electric and magnetic dipoles associated with enantiomers and chiral plasmonic

49 at accounted for interactions of neighboring dipoles at either an aligned or opposed possible orienta

50 rical stimuli showed different short-latency dipoles between the two age groups, and the juveniles la

51 Cl), XS, it was found that the effect of the dipole-bound (DB) electron on the cage intramolecular co

52 The role of long-lived dipole-bound resonances built on the singlet state below

53 Excited dipole-bound states (DBSs) are uncovered for the three a

54 art leads to the formation of a non-valence (dipole-bound) state.

55 incommensurate helical ordering of electric dipoles by light hole doping of the quadruple perovskite

56 We review emerging evidence that climate dipoles can entrain species dynamics and offer a framewo

57 ontrasts the multitude of strong pai-cation, dipole-cation, and ion-pair interactions between all int

58 ta-atoms can have both electric and magnetic dipole characteristics (and hence radiation properties),

59 to optimizations based on just one specific dipole class, the electrophilicity of the alkynes in SNO

60 source density analysis revealed HFO current dipoles close to the mitral layer and unit firing of mit

61 RET, and rotational diffusion of fluorophore dipoles, complicate interpretation of FRET data and have

62 involving coadsorption of a strong molecular dipole compound with a chromophore, is a versatile metho

63 n enhancement of molecular ordering of water dipoles, consistent with the observed behavior at the gl

64 show an elegant implementation with just two dipole-coupled magneto-tunneling junctions (MTJ), with m

65 ine a simplified metric (EMOD1) that weights dipole coupling as a function of distance and relative o

66 The effect of dipole coupling can be varied by generating local strain

67 nerates the anti-correlation with "wireless" dipole coupling that consumes no footprint on a chip and

68 emical force (hydrogen bonding) and magnetic dipole coupling to assemble polymer-brush coated superpa

69 cond MTJ's resistance state is determined by dipole coupling with the first, thus correlating the sec

70 in Ni or Terfenol-D systems due to its large dipole coupling.

71 a longer emitting wavelength due to reduced dipole (D(+*) ->A(-*) ) size, enhanced SOC, increased or

72 charge-transfer occurs with forming electric dipoles (D(+*) ->A(-*) ), providing the ionic polarizati

73 NDI-NI showed a higher interfacial dipole (Delta), conductivity, and electron mobility than

74 randomized UNCOVER AF trial (Utilizing Novel Dipole Density Capabilities to Objectively Visualize the

75 patients showed significantly reduced source dipole density of gamma-band ASSR (ITC > 0.25) in the le

76 ies of many magnetic materials consisting of dipoles depend crucially on the nature of the dipole-dip

77 prominent ion-modifier interactions: charge-dipole, dipole-dipole, and charge-quadrupole.

78 onsequence of a competition between magnetic dipole-dipole and ligand interactions.

79 rophilic PEG tails in a nonpolar solvent and dipole-dipole attraction between NCs, drive mesoscale as

80 hesize that the merging process is caused by dipole-dipole coalescence between the daughter droplets.

81 find that we can precisely control both the dipole-dipole coupling between nanoparticles and the str

82 Stronger dipole-dipole coupling can mediate excitonic coupling in

83 FRET is mediated by weak Coulombic dipole-dipole coupling of donor and acceptor fluorophore

84 y study the effect of spin-orbit coupling on dipole-dipole energy transfer in MOFs using steady-state

85 he exit-channel region due to the long-range dipole-dipole interaction between the nascent radical pr

86 s(merocyanine) dyes allows one to direct the dipole-dipole interaction driven aggregation into stacks

87 The results indicate dipole-dipole interaction strengths at the 100 to 200 K

88 ipoles depend crucially on the nature of the dipole-dipole interaction.

89 ocess became possible due to the predominant dipole-dipole interactions among MC dyes that allowed fo

90 a*((C-X)) orbital or the minimization of the dipole-dipole interactions are currently the two leading

91 The strong dipole-dipole interactions in polar molecule(5) and Rydb

92 using the rich interplay of photon-mediated dipole-dipole interactions in structured subwavelength a

93 ise control of dye assembly via hierarchical dipole-dipole interactions opens the door for a more pre

94 t L-shape conformations, generating stronger dipole-dipole interactions resulting in shorter inter-ch

95 Remarkably, we find that strong dipole-dipole interactions stabilize the dark condensate

96 confirm the theoretical predictions that the dipole-dipole interactions together with the external ma

97 to water-mediated modulation of ion-induced dipole-dipole interactions.

98 ent spin state, under the effect of magnetic dipole-dipole interactions.

99 molecular rotors differing in intramolecular dipole-dipole spacing was synthesized.

100 nt ion-modifier interactions: charge-dipole, dipole-dipole, and charge-quadrupole.

101 ar dispersion implies that geomagnetic axial dipole dominance averaged over 10(7)-10(9) years has rem

102 ic poles at the equator and the median axial dipole dominance measured at Earth's surface.

103 much less is known about the degree of axial dipole dominance.

104 loss lithium niobate piezoelectric electric dipole driven at acoustic resonance that radiates with g

105 We investigated influences of the dipole-driven orientation and resulting directional conf

106 eic anhydride experiences a larger change in dipole during the reaction-leading to a larger solvent d

107 sult of the coherent superposition of atomic dipole emissions.

108 erties of a solid through combined action of dipole excitation and field dressing.

109 based on the directional emission of Huygens dipoles excited in an individual dipolar antenna.

110 Hirshfeld charge analysis indicates that dipole fields from oriented imine linkages within COF-42

111 o that of other frequency bands and standard dipole fitting methods.

112 mating that expected from a geocentric axial dipole for the interval 8 to 11 million years ago, but w

113 erate the highly reactive palladium-mediated dipoles for the first time, and a diverse array of stabl

114 novel spiroannulation of exo-imines with 1,3-dipoles, for the first time, leading to 3D spirocycles w

115 ne is completely dark, the other one is only dipole forbidden out-of-plane, hence referred to as grey

116 energy paipai* excited state instead of the dipole-forbidden npai* state, the quantum yield of isome

117 , both interatomic radiative transitions and dipole-forbidden transitions can become comparable to th

118 ed in a focused laser beam will experience a dipole force due to the gradient in the interaction ener

119 We show that the velocity dependence of the dipole force is cancelled out by another force that is r

120 Molecular dipoles from simple organic functional groups (amide, ur

121 an electron or hole by extended ordering of dipoles from symmetry-broken unit cells.

122 tructural models through an analytical point-dipole Hamiltonian for the hydride electron-nuclear dipo

123 (12) In analogy with magnetism, the electric dipole helicoidal texture is stabilized by competing ins

124 ecreases as theta(e) increases, along with a dipole-hexadecapole transformation, which are confirmed

125 Here, we identify a north-south dipole in annual climatic moisture deficit anomalies acr

126 terms of the stabilization of the developing dipole in the transition state.

127 Long-range ordering of magnetic dipoles in bulk materials gives rise to a broad range of

128 The role of climate dipoles in shaping ecological and evolutionary processes

129 ynamics describing generation of local force dipoles in the junctional actomyosin.

130 suming perfect, polar alignment of molecular dipoles in the nematic.

131 al "ice rules," in analogy with the electric dipoles in water ice.

132 ce sink-source compensation between regions (dipoles) in atmospheric inversion so that their estimate

133 cle increases (i.e., >=80 nm), the number of dipoles increases, which results in higher dipole-multip

134 These results suggest that the dipole-induced dipole interaction was dominant, and that

135 Additionally, dipole-induced energy-level realignment between the two

136 d on the existence of an "effective electric dipole" inspired by recent reported structures of lyseni

137 on in NML relies on Bennett clocking through dipole interaction between neighboring nanomagnetic bits

138 Increasing the dipole interaction between particles by increasing parti

139 When the dipole interaction is dominant the rotors swing upwards

140 hese results suggest that the dipole-induced dipole interaction was dominant, and that maltose-with t

141 (by hydrogen bonding with AOT anion and ion-dipole interaction with BHD(+)) between the entrapped wa

142 ne-dimensional (1D) dipole pairs, induced by dipole interaction, regulate the conductivity, as well a

143 t in monolayer owing to the large unscreened dipole interactions and suppression of charge-transfer p

144 bilization of charged sites is due to charge-dipole interactions mediated by the large dipole moment

145 competition of the exchange and the magnetic dipole interactions, the minimum-energy magnon state is

146 tori together as a result of [K(+)...O] ion-dipole interactions.

147 solid ferromagnets with classic north-south dipole interactions.

148 field effects are enhanced by nonlocal image-dipole interactions.

149 fields (LEFs), i.e., by embedding charges or dipoles into molecules.

150 The Indian Ocean Dipole (IOD) affects climate and rainfall across the wor

151 The imprint of this climatic dipole is manifest for years postfire, as evidenced by d

152 on path using our water flooding and protein dipole Langevin dipole semimacroscopic formalism with it

153 e gating effect of a Li-adsorption-generated dipole layer at the ZrTe(5) surface.

154 helical hexapeptides to establish a surface dipole layer on a TiO(2) substrate, with the goal of inf

155 As an interfacial dipole layer, the PFE polymer plays a critical role in i

156 parallel orientations to the surface lead to dipole-like or quadrupole-like defect structures.

157 Using inelastic X-ray scattering beyond the dipole limit and hard X-ray photoelectron spectroscopy w

158 d Hall measurement using a rotating parallel dipole line system and an equation, Deltamu(H) = d(sigma

159 Arctic Ocean, not unlike those of the Arctic dipole linked to the recent loss of Arctic sea ice.

160 icant due to the high density of oscillating dipoles localized on the corners.

161 first-principles theory, further supporting dipole locking at AP.

162 The dipole magnetic fields of the NV-resonant magnons couple

163 inear energy dispersion and large transition dipole matrix element, graphene is an attractive materia

164 to factors lowering steric repulsion and/or dipole minimization.

165 se-Einstein condensate (BEC), where the spin-dipole mode (SDM, actuated by quenching the Raman coupli

166 fies [Formula: see text], the point electric dipole model becomes accurate.

167 onforms to either the hard-sphere or induced-dipole model.

168 lled not only by the "critical" value of the dipole moment (mu > 2.5 D), but also by a geometric fact

169 d provides the basis for determining the ion dipole moment and direction within the molecular frame f

170 ew theoretical constructs, which include the dipole moment and interfacial polarizability.

171 ge-dipole interactions mediated by the large dipole moment and the low volatility of sulfolane.

172 ically disordered organic cations with large dipole moment benefit the optoelectronic properties of C

173 that relates the rotation of the transition dipole moment between reversible E->Z photoisomerization

174 tark spectra revealed dramatic light-induced dipole moment changes in the range [Formula: see text] =

175 e diffusive light is based on ~15-ps initial dipole moment depolarization followed by ~50-ps repolari

176 tes were determined by the difference of the dipole moment in each saccharide.

177 indirect excitons with a permanent electric dipole moment in heterobilayer crystals promise realizat

178 bes the tendency of a molecule to change its dipole moment in response to an applied electric field.

179 iourea groups introduce a localized electric dipole moment into the SAM and change the polarizability

180 concomitant annihilation of the ground state dipole moment is observed in the UV/vis absorption spect

181 Consequently, the internal dipole moment of an individual molecule can be spatially

182 of a sodium-pump rhodopsin (KR2) by altering dipole moment of residues around the retinal chromophore

183 show strong solvatochromism due to the large dipole moment of the ground states and the transition di

184 The dipole moment of triafulvene of 1.90 D suggests that thi

185 oscopic analysis reveals that the transition dipole moment orientation of bright excitons in the supe

186 tion bands are characterized by a transition dipole moment oriented along the short acene axes, in th

187 onic structure aligns the exciton transition dipole moment parallel to the surface plane, thereby out

188 A detailed study on the ultrafast dipole moment reorientation dynamics demonstrates that r

189 ull-dimensional ab initio WHHB potential and dipole moment surfaces.

190 st for state-of-the-art water potentials and dipole moment surfaces.

191 ment of the ground states and the transition dipole moment that is in the opposite direction.

192 tation is conditioned by the response of its dipole moment to environmental electrostatic changes.

193 is governed by the rate of increase of their dipole moment with the shortening of the dative Si <- N

194 Hall effect provides a direct measure of the dipole moment(10) of the Berry curvature, which arises f

195 Each structure features a permanent dipole moment, generated by an N,N-dimethylamino- moiety

196 s dominant, and that maltose-with the higher dipole moment-was more strongly retained compared to oth

197 en mirror symmetry and an intrinsic vertical dipole moment.

198 compared to other disaccharides having lower dipole moment.

199 den optical transitions with an out-of-plane dipole moment.

200 enhancement of a measurable atomic electric-dipole moment.

201 character with a large charge separation and dipole moment.

202 face chemistry in accordance with the enzyme dipole moment.

203 st absorbed by excitations carrying electric dipole moment.

204 rk for state-of-the-art water potentials and dipole-moment surfaces, especially with respect to three

205 750 eV (2270 and 6050 cm(-1)) and transition dipole moments (Deltamu = 13-18 D) that are among the hi

206 While optical transition dipole moments (TDMs) in zero to two-dimensional optical

207 tion of the electric and magnetic transition-dipole moments between the lowest electronic states of t

208 Water dipole moments calculated using polarizable force fields

209 fraction of horizontally aligned transition dipole moments compared to (dbx)Pt(dpm) doped into a 4,4

210 increase in horizontally aligned transition dipole moments compared to the film deposited in the abs

211 ization change consistent with the change in dipole moments during the VT process.

212 terlayer excitons with out-of-plane electric dipole moments in opposite directions.

213 ns of the excitation and emission transition dipole moments in the FPs mTurquoise2, eGFP, and mCherry

214 y demonstrate that a change in the molecular dipole moments induced by intramolecular electron transf

215 The dipole moments obtained from threshold fields for alignm

216 on is important for measurements of electric-dipole moments of atoms, which would indicate CP violati

217 after equal times increase linearly with the dipole moments of chloro-, nitro- dichloro-, and dinitro

218 tatic instability arising from the intrinsic dipole moments of polar facets, however, leads to differ

219 Nucleobase dipole moments vary as a function of position and also c

220 assumed that we are in the regime of strong dipole moments where a classical treatment is possible.

221 ing molecular building blocks that have bond dipole moments with spatial orientations that favor anti

222 ing to lower free energy barriers and higher dipole moments.

223 e rotational structure of the molecules with dipole moments.

224 ilize systems with larger, more polarizable, dipole moments.

225 Examples range from dipole, monopole, and patch antennas for far-field RF op

226 f dipoles increases, which results in higher dipole-multipole interactions.

227 om the electrostatic interaction between the dipole of *CO[Formula: see text] and the interfacial fie

228 (3) moiety-the positive end of the molecular dipole of XS.

229 between the electric and magnetic transition dipoles of the polymer donor and superhelicene acceptor,

230 zable polarization, ~10 muC/cm(2) due to the dipoles on the organic.

231 glass-i.e., by probing its response to force dipoles-one can disentangle and independently extract th

232 e, electronic distribution, polarity, pK(a), dipole or polarizability, which can be either favorable

233 s charge density wave (CDW) and magnetic and dipole ordering, have potential to be exfoliated into mo

234 nsition materials with CDWs and magnetic and dipole ordering, including transition metal dichalcogeni

235 The relative dipole orientation between the GFPs is best described by

236 , emission spectrum, and in-plane excitation dipole orientation of CdSSe/ZnS quantum dots suspended i

237 The dipole orientation of ground-state Gamma-K interlayer ex

238 ces ion migration, reports on the sensitizer dipole orientation, and (in some cases) reorients or fli

239 hotonic chips which exploit the out-of-plane dipole orientation.

240 naturally occurring out-of-plane luminescent dipole orientation.

241 ponded to changes in the in-plane excitation dipole orientation.

242 states to two different permanent electrical dipole orientations generated from the Gd atom being tra

243 It is demonstrated that one-dimensional (1D) dipole pairs, induced by dipole interaction, regulate th

244 k chemistry that uses mesoionic compounds as dipole partners.

245 through a feedback mechanism that excites a dipole pattern in vertical wind shear (VWS), a metric th

246 This suggests the dipole pattern is robust, and one mode may be favored fo

247 Here we show that a dipole pattern of similar geographic extent persisted an

248 ently characterized by a north-south wet/dry dipole pattern, controlled by interaction of the storm t

249 The molecular dipole polarizability describes the tendency of a molecu

250 uantum mechanical calculations of the static dipole polarizability tensors of 7,211 small organic mol

251 ectric materials that have a quasi-permanent dipole polarization.

252 ded emitters and allow the reconstruction of dipole positions with 1-nm precision.

253 lar to apolar media), accurate transmembrane dipole potential, and diffusion under periodic boundary

254 ected to a moving spin-independent repulsive dipole potential.

255 he first time, and a diverse array of stable dipole precursors was explored for the elaboration of ch

256 ces to lock the permanent macromolecular ion dipoles, producing novel separations based solely on the

257 gurations at zero temperature for systems of dipoles ranging from small to an infinite number of part

258 bda ~ 15%) mode shifting between an electric dipole resonance and an anapole state.

259 etermined by localized magnetic and electric dipole resonance of nanostructures, which are sensitive

260 ion mechanism due to the presence of surface dipoles resulting in a power conversion efficiency (PCE)

261 possible orientation of the local threefold dipole rotation potentials within a channel of the TPP h

262 erroelectric domain switching and continuous dipole rotation.

263 Among the dipoles routinely used for click chemistry, azides, nitr

264 s the magnitude and orientation of molecular dipole(s), as well as the arrangements of chromophores o

265 n modes for a system composed of two coupled dipole scatterers.

266 ion; and, secondly, the breaking down of the dipole-selection rule for radiative transitions in isola

267 r water flooding and protein dipole Langevin dipole semimacroscopic formalism with its linear respons

268 The presence of the peptide molecular dipole shifted the HOMO levels of the ZnTPP group to low

269 d controversial because of the poor electric dipole stability in single molecules.

270 The two dipole states are separated by a transition energy barri

271 ectret is the switching between two electric dipole states by an external electric field.

272 The maximum generator dipole strength was about 24 uA-cm.

273 Reported here is a molecular dipole that self-assembles into highly ordered patterns

274 f panels with different patterns of magnetic dipoles that are capable of specific binding.

275 ions suggest the Michael addition of the 1,3-dipole to be the rate- and enantiodetermining step, and

276 ation through intermolecular charge-transfer dipoles to harvest nonradiative triplets into radiative

277 trengths at the 100 to 200 K scale that lead dipoles to preferentially populate a subset of low-energ

278 the energy landscape markedly and allow the dipoles to rotate continuously between the a and c nanod

279 s orient around 98% of the neighboring water dipoles toward the protein surface, and such correlation

280 ic fields in electronic materials can induce dipole transitions between eigenstates or distort the Co

281 It is shown that electric dipole transitions can be enhanced near the focus of a d

282 re light-matter interactions beyond electric dipole transitions.

283 ough state-dependent atom loss in an optical dipole trap of ultracold (6)Li atoms.

284 offer a framework for identifying ecological dipoles using broad-scale biological data.

285 ing the electric field generated by cortical dipoles using realistic finite element modeling.

286 c phosphoramidite as supporting ligand, this dipole was applied to the asymmetric synthesis of chiral

287 A novel palladium-mediated carbonylogous 1,4-dipole was developed by in situ deprotonation.

288 Resulting 1,3-dipole was trapped with fluoroalkenes, fluoroalkylated a

289 in contrast with the in-plane orientation of dipoles we find in two-dimensional WSe(2) and MoSe(2) at

290 f individual quantum dots and the excitation dipoles were visualized in the context of structural fea

291 e present work, we study systems of magnetic dipoles where the dipoles are arranged on various types

292 cent geomagnetic field is its dominant axial dipole which provides its navigational utility and dicta

293 from the stacking sequence of the molecular dipole, which is reoriented by the electric field betwee

294 erials show electrically switchable electric dipoles, which are usually formed by spatial separation

295 uthwestern US (SW) track the strength of the dipole, while declining overall due to increasing aridit

296 ic core structures derived from 1,3- and 1,5-dipoles; while reaction with cyclic dienes yields severa

297 The model predicts an elastic dipole whose stability decreases as theta(e) increases,

298 nological records to correlate this climatic dipole with short-term postfire juvenile recruitment.

299 f positive charges in film materials forming dipoles with the F4TCNQ radical counteranions.

300 s with preference for the Re face of the 1,3-dipole, with formation of a diastereomeric mixture in 73