ライフサイエンスコーパス: bond length

1 strength, with emphasis on the importance of bond length.

2 xygen positions and the often neglected Si-O bond length.

3 ate description of the bond strength via the bond length.

4 f freedom, increases with increasing valence bond length.

5 ether with their binding energies, and their bond lengths.

6 deling to result in unheard of carbon-oxygen bond lengths.

7 state, hybridization state, and metal-ligand bond lengths.

8 er of hydrogen bonds having relatively short bond lengths.

9 the S(0) and (1)pisigma* PESs at longer O-H bond lengths.

10 lity in these systems is limited to about 24 bond lengths.

11 delocalization interactions in impacting O-P bond lengths.

12 ty of the scissile O-P bond through computed bond lengths.

13 ith a square planar geometry but with longer bond lengths.

14 stituent) are shown to result in shorter O-P bond lengths.

15 ly the same quadratic dependence as the Ln-X bond lengths.

16 d on their measured and our calculated Zn-Zn bond lengths.

17 ter of which can be used to infer (1)H-(17)O bond lengths.

18 While the O-O bond length (1.462(3) A) barely changes upon protonation

19 The V-NE2 bond length (2.25 A) suggests that VO(3) is not covalent

20 The Cl-O bond length (2.98 A) for Cl(-)/H(3)O(+) is approximately

21 The isostructural chloroxenate anions (Xe-Cl bond lengths, 2.9316(2) to 3.101(4) A) were synthesized

22 ccupancy of the Fe 3d orbital; a longer Fe-O bond length; a decreased covalency of the Fe-O bond; and

23 associated rate strongly correlates with the bond length alternation (BLA) of the two bridge bonds.

24 A detailed structure-property correlation of bond length alternation data and Raman frequencies is pr

25 s-retinal isomers) is due to the decrease in bond length alternation of the retinal.

26 This result suggests that a decrease in bond length alternation results in an increase in antiar

27 then introduce a Marcus-Hush model with the bond length alternation vibrational mode, treating the G

28 nd length alternation, which showed that the bond length alternation was slightly greater for the ant

29 , when structures of 5(2-) and 5(2+) with no bond length alternation were examined, there was a drama

30 in acetonitrile vs 1777 cm(-1) for BTP) and bond length alternation within its benzenoid ring.

31 ed states have high cumulenic character (low bond length alternation) around the central region of th

32 ondon region dominated by changes in retinal bond length alternation, (2) dwell time on the excited s

33 s the electron delocalization, decreases the bond length alternation, and leads to variation in the w

34 nduced charge transfer, and reduction of the bond length alternation, as well as smaller Gibbs energi

35 the TES-ethynyl groups in 1 lead to enhanced bond length alternation, resulting in weaker aromaticity

36 examined through comparison of the degree of bond length alternation, which showed that the bond leng

37 the absence of any significant carbon-carbon bond-length alternation (BLA) along their backbones.

38 le, [3]TrTol, outline monotonic increases in bond-length alternation (BLA) upon stepwise reduction.

39 -)) in the active site induce changes in the bond-length alternation of the all-trans retinyl chromop

40 43 nm spectral shift is due to an increased bond-length alternation of the protonated Schiff base of

41 mbining the donor-acceptor strategy with the bond-length alternation reduction strategy.

42 alculated bond lengths reveal a reduction in bond-length alternation upon photoexcitation, indicating

43 The response of the structural (bond-length alternation, rotational barrier) and molecul

44 the sum of van der Waals radii) and that the bond-length-alternation is perturbed in the vicinity of

45 Bond length analysis and XPS studies of Ce(33)Fe(13)B(18

46 nounced electronic changes as evidenced by a bond length analysis.

47 n diffraction results, along with supporting bond-length analysis from high resolution x-ray diffract

48 perties of the spacers can be predicted from bond length and conformation data (obtained from crystal

49 e in ionization potential and an increase in bond length and decrease in acceptor aromaticity.

50 Engineering molecules with a tunable bond length and defined quantum states lies at the heart

51 ll-known relationship between bond order and bond length and makes use of the experimental bond dista

52 ound state as linear 3Sigma(u)+ with 1.840 A bond length and molecular orbital occupancies for an eff

53 sts revealed no correlation between the Ru-O bond length and Ru-O bond strength.

54 nce-to-core XES peak was correlated with N-N bond length and stretching frequency.

55 nifested by the pronounced elongation of O-C bond length and the tilting of the methoxy axis, which f

56 r, subject to larger deformation of the Pb-X bond length and X-Pb-X bond angles, sees the formation o

57 rine ring structure yielded the experimental bond lengths and 2sigma errors R(B-N) = 1.45(3) A, R(B-C

58 state is accompanied by an increase in Fe-N bond lengths and a concomitant contraction of intraligan

59 onding geometry (by maintaining the original bond lengths and angles and omega dihedrals).

60 Trends in crystallographic bond lengths and angles shed light on the structural cha

61 iene) afforded 1-[Ir(COD)Cl], a complex with bond lengths and angles that were in accord with known N

62 sitions can cover all of the known ranges of bond lengths and bond angles for a given type of metal c

63 omers for each series were computed, and the bond lengths and bond angles were calculated.

64 l volume, as well as in specific interatomic bond lengths and bond angles.

65 based on the precise structural parameters (bond lengths and coordination number) extracted from the

66 Further, the requirement for identical Cu-Se bond lengths and Debye-Waller factors at each absorption

67 ve been published, reporting a wide range of bond lengths and dissociation energies.

68 nd 300 K also reveals elongation of the Fe-P bond lengths and increment in the Cl-Fe-Cl angle as the

69 large deviation from the correlation of C-C bond lengths and strengths, but the computed force const

70 have a dramatic influence on alkylperoxo O-O bond lengths and the barrier to alkylperoxo O-O bond cle

71 3 calculations on 1a-c provided quantitative bond lengths and torsional angles to support the conclus

72 compounds with relatively short Fe-N(imide) bond lengths and two-electron reduction of the redox-act

73 ns is provided by a geometry optimization of bond lengths and valence angles with XRD torsion angles

74 al symmetry, microstrain, and effective 'DNA bond' length and strength.

75 , Omega = 3) ground state, a similar 1.855 A bond length, and a fully developed triple bond of 2.82 e

76 he potential impact of charge, metal-iridium bond length, and stability of terminal vs internal alken

77 rotation angles, packing distances, hydrogen bond lengths, and helical pitches) for the one and three

78 We assess covalent geometry by determining bond lengths, angles, dihedrals and rotamers.

79 nt collapse process didn't induce volume and bond length anomalies in the two compounds, the unique a

80 nformational changes in DNA structure as the bond length approaches 3 nm and show that cations that s

81 and width, orbital overlap, bond energy, and bond length are used to explain trends in electronic pro

82 Phosphoryl bond lengths are found to correlate strongest (R = 0.90)

83 though deviations from ideal bond angles and bond lengths are frequent(6), alternative parent geometr

84 xes, [Titm(Me)]ZnX, demonstrate how the Zn-C bond lengths are highly variable (2.17-2.68 A) and are u

85 culated incorporation energies and optimized bond lengths are presented.

86 Bk(III)-O and Bk(IV)-O bond lengths are shorter than anticipated and provide fu

87 ion states are also highly asynchronous, but bond lengths are skewed in the opposite direction compar

88 ction induces substantial contraction in all bond lengths around the metal centers, along with diagno

89 The sum of all bond lengths around the trivalent metal cation, however,

90 etermination of the individual Zn-N and Zn-C bond lengths as 1.969(2) and 2.030(2) A, respectively.

91 irst breakthrough in direct C-H and C[double bond, length as m-dash]C bond alkynylation has also been

92 lic configurations; the presence of C[double bond, length as m-dash]C bonds and aromatic rings; and f

93 al addition of a hydrogen atom to a C[double bond, length as m-dash]C double bond.

94 metallacyclocumulenes Cp'2M[eta2-C(R)[double bond, length as m-dash]C(C2R)-C(R)[double bond, length a

95 ash]C[double bond, length as m-dash]C[double bond, length as m-dash]C(R)-] (formed by coordination of

96 ash]C[double bond, length as m-dash]C[double bond, length as m-dash]C(R)-] (formed by coordination of

97 -C(R)[double bond, length as m-dash]C[double bond, length as m-dash]C(R)-C(R2)-] (formed by coordinat

98 SiC2SiMe3 (mono-functional alkynes: C[triple bond, length as m-dash]C) in Cp'2M(eta2-Me3SiC2SiMe3) (C

99 C[triple bond, length as m-dash]C, C[triple bond, length as m-dash]C), and seven-membered metallacyc

100 C[double bond, length as m-dash]C, C[double bond, length as m-dash]C), five-membered metallacycloall

101 C[double bond, length as m-dash]C, C[triple bond, length as m-dash]C), metallacyclocumulenes Cp'2M[e

102 C[triple bond, length as m-dash]C, C[triple bond, length as m-dash]C), with M = Ti, Zr, and Hf were

103 dination of tri-functional trienes: C[double bond, length as m-dash]C, C[double bond, length as m-das

104 C[double bond, length as m-dash]C, C[double bond, length as m-dash]C, C[double bond, length as m-das

105 ordination of bi-functional enynes: C[double bond, length as m-dash]C, C[triple bond, length as m-das

106 ordination of bi-functional diynes: C[triple bond, length as m-dash]C, C[triple bond, length as m-das

107 nation of two bi-functional diynes: C[triple bond, length as m-dash]C, C[triple bond, length as m-das

108 di-Ph2P- (hetero-tri-functional: P, C[triple bond, length as m-dash]C, P) in Cp'2M(eta2-Ph2C2PPh2), a

109 ha-mono-SiH- (hetero-bi-functional: C[triple bond, length as m-dash]C, SiH) and alpha-di-SiH-substitu

110 lkynes (hetero-tri-functional: SiH, C[triple bond, length as m-dash]C, SiH) in Cp'2M(eta2-Me3SiC2SiMe

111 d metallacycloallenes Cp'2M[eta2-C(R)[double bond, length as m-dash]C[double bond, length as m-dash]C

112 metallacyclocumulenes Cp'2M[eta2-C(R)[double bond, length as m-dash]C[double bond, length as m-dash]C

113 -C(R)[double bond, length as m-dash]C[double bond, length as m-dash]C[double bond, length as m-dash]C

114 le bond, length as m-dash]C(C2R)-C(R)[double bond, length as m-dash]C[double bond, length as m-dash]C

115 -C(R)[double bond, length as m-dash]C[double bond, length as m-dash]C[double bond, length as m-dash]C

116 contributions of the carbene (LAu(+)[double bond, length as m-dash]CR2) and alpha-metallocarbenium (

117 Formazans (Ar1-NH-N[double bond, length as m-dash]CR3-N[double bond, length as m-da

118 ash]O units has been replaced by an S[double bond, length as m-dash]N moiety, they can confer new rea

119 N[double bond, length as m-dash]CR3-N[double bond, length as m-dash]N-Ar5), a class of nitrogen-rich

120 /elaborated for the generation of [An[double bond, length as m-dash]NR] and [Ln[double bond, length a

121 le bond, length as m-dash]NR] and [Ln[double bond, length as m-dash]NR] moieties.

122 es of sulfones where one of the two S[double bond, length as m-dash]O units has been replaced by an S

123 red as a metric of N(2) reduction to the N-N bond length, as there is excellent agreement between the

124 in vacuum and direct measurements of the C-C bond lengths at the edge show ~86% contraction relative

125 hat are unsupported by bridging ligands, the bond lengths being calculated as 3.229 A for [Re2Cp2(CO)

126 stronger adsorption energy and shorter Fe-O bond length between 2H-AgFeO(2) and -OH.

127 delocalized structure with no difference in bond length between adjacent C(meso)-C(alpha) bonds.

128 als with a step of 0.5 nm, comparable to the bond length between two adjacent DNA bases.

129 Bond lengths between pairs of atoms in covalent molecule

130 is observed, which can be used to determine bond lengths between selected pairs of equivalent atoms

131 In addition, there is a trend toward longer bond lengths between the C(2) ketal center and the aryl

132 ional modes originate from the change of the bond lengths between the metal atoms and chalcogen atoms

133 inated structure with a wide distribution of bond lengths, bond angles, and five-, six-, seven- and e

134 verse-kinematics approach and assuming fixed bond lengths, bond angles, and peptide bond torsions, as

135 The backbone bond lengths, bond angles, and planarity of a protein ar

136 t 13C' CSA tensors are sensitive to hydrogen-bond length but not hydrogen-bond angle.

137 NMR spectroscopy reveals a very short H-H bond length, but the hydrogen molecule is activated towa

138 structural sensitivity to the corresponding bond lengths, but previous studies have failed to identi

139 ette's sultam resulted in an increase in S-N bond length by ca. 0.06 angstrom.

140 mplex molecule via changing the metal-ligand bond length can shift its electronic energy levels and p

141 s static and dynamic disorder in metal-metal bond lengths can be obtained.

142 This difference in Fe-S bond lengths can be understood in terms of variations in

143 ese dizinc products also provide their Zn-Zn bond lengths: CCSD(T) calculations find a short 2.367 an

144 e modulated by the probe energy and that the bond length change associated with molecular breathing m

145 The Co-O transient bond length changes and the optical spectra and kinetics

146 The bond-length changes in the Mn(CO) 3 moiety were much lar

147 between CO and O with a distribution of OC-O bond lengths close to the transition state (TS).

148 a 0.018 A decrease in C(delta)-H/C(gamma)-O bond length, consistent with favorable sigmaC-H --> sigm

149 ](+) complex exhibits symmetric Mn-O(peroxo) bond lengths, consistent with a side-on bound peroxo lig

150 us relaxations, involving large out-of-plane bond length contractions for the edge atoms (approximate

151 e scattering environments with corresponding bond lengths, coordination numbers, and Debye-Waller fac

152 nts in annual reproductive success with pair-bond length could be a secondary factor favouring perenn

153 es the difference between long and short V-V bond-lengths (Delta(V-V)) in monoclinic structures which

154 anthanide contraction in the individual Ln-O bond lengths deviates considerably from the expected qua

155 Analysis of B-F bond lengths (DFT) in the intermediate difluoroborane, o

156 The C-C bond lengths differ by only 0.028 angstrom, indicating v

157 the hopping integral to simulate structural (bond-length) disorder.

158 ents, we show that these results support the bond length disproportionation model of the MIT in the r

159 The bimodal bond-length distributions observed here are shown to cau

160 arly resolved, with observable variations of bonding lengths due to excess Coulomb force from bare io

161 dies and DFT calculations show that the Pb-I bond length elongation reduces the overlap of the Pb s-

162 ack as reflected by free energy, C1-O1/O5-C1 bond length elongation/reduction, C1-O1 bond orientation

163 usually found in aromatic compounds such as bond length equalisation, energetic stabilisation, and p

164 jugated structures near the cyanine limit of bond length equalization as a result of the strong inter

165 ructural Database turned up no bona fide C-O bond length exceeding this value.

166 spin states as functions of the metal-oxygen bond length for a Co(3+) ion in an octahedral coordinati

167 The bond lengths for 19 and 27 were consistent with the pres

168 A comparison of CH bond lengths for geometrically relaxed uracil molecules

169 persion correction resulted in shortened M-C bond lengths for the stable complexes, and it was found

170 Halogen bond lengths for these units, observed by single crystal

171 n ground state structures, from noncanonical bond lengths for WT toward solution values with mutants.

172 At specific O-O distances, consistent with bond lengths found in amorphous Al2O3 or near Al2O3 surf

173 one of the bonding subgroups (with the same bond length) found in amorphous PCMs, in marked contrast

174 ddition can be used to controllably tune DNA bond length from 16 to 3 nm and to increase bond stabili

175 ere we demonstrate the retrieval of multiple bond lengths from a polyatomic molecule by simultaneousl

176 n these complexes and may help deduce the NO bond lengths from using experimental vibrational data in

177 eme in both structures is the elongated Pt-P bond lengths (>2.4 A), indicating that nucleophilic liga

178 The charges on the atoms and bond lengths have been calculated using natural bond orb

179 roximately 0.1 A longer than the average U-C bond length in 1 (2.522(2) A).

180 y crystallography, which showed that the U-C bond length in 2 (2.624(4) A) is approximately 0.1 A lon

181 A slight increase of the Co-Co bond length in 2 is more likely to be caused by the stro

182 AFS) simulations indicate the average Fe-O/N bond length in Dfh is 2.13 A, consistent with a ligand g

183 Moreover, the nearest-neighbor Fe-Se bond length in SC samples exceeds that in the non-SC (NS

184 The Mo-Mo bond length in the Mo2O10 dimers is 2.684(8) A, while th

185 is electrostatic arrangement affects the N-H bond length in the region of the flavin reactive center.

186 We additionally show that the O-H bond length in these catalysts can be measured with sub-

187 g the Fe-O stretching frequency and the Fe-O bond length in this excited state and quantifying the pi

188 by simultaneously measuring the C-C and C-H bond lengths in aligned acetylene.

189 nship between NO vibrational frequencies and bond lengths in all of these NO-containing systems.

190 laining this non-classical trend of the An-L bond lengths in both series, underscoring the significan

191 Intriguingly, the flavin bond lengths in oxidized GR are intermediate between tho

192 a smaller singlet-triplet splitting, closer bond lengths in the ground (1)A' and the first excited (

193 Longer C(spiro)-O bond lengths in the SO form and slower rates of thermal

194 We illustrate the method by determining the bond lengths in the structure of the Co(II) coordination

195 The absence of differences in intraligand CC bond lengths in the transition states relative to the gr

196 accounts for the different O-O, S-S, or S-O bond lengths in the triatomic series.

197 An analysis of bond lengths in these systems by X-ray crystallography a

198 ue to the charge disorder and fluctuation of bonding length in Ln(3) NbO(7) plays a major role.

199 ochronicity was no longer apparent beyond 17 bond lengths (in 24c).

200 I(t)BuPrCO(2) (2f) indicate that the C-CO(2) bond length increases as the N-substituents rotate towar

201 The shorter bond length indicated that the solution contained a bide

202 eatures a virtually planar central ring with bond lengths indicating significant delocalization.

203 d CaCO(3) but with much larger C-O and Ca-Ca bond lengths, indicating a lower density and a mechanism

204 I fluorescent state featuring an untwisted, bond length inverted RPSB, and (3) rapid torsional evolu

205 r the complex, the experimental ethylene C-C bond length is 1.432(5) A, which falls between the free

206 The Fe(IV)-O unit bond length is 1.680(1) A, which is the longest distance

207 While the Te-Pt bond length is only slightly affected by the oxidation s

208 re of 3-t-Bu reveals that the trans U-O(ArO) bond length is shortened by 0.1 A in comparison to the c

209 In contrast, the N-I bond length is virtually unaffected by changes of the el

210 hermore, the difference in Hg-EPh and Cd-EPh bond lengths is a function of the chalcogen and increase

211 AdoCbl structure, and specifically the Co-C bond length, is not a basis of Co-C bond cleavage cataly

212 um dots registered to within a single atomic bond length (limited by the polydispersity of the quantu

213 he cooperative effects of changes in the V-O bond length, localization of V(3+) electrons at V(5+) si

214 ue series of ruthenates in which the average bond length <A-O> remains the same but the bond-length v

215 c SrRuO3 can be obtained from the curve at a bond length <A-O>, which makes the geometric factor t =

216 onstrate a parabolic curve of Tc versus mean bond length <A-O>.

217 Changes as small as 0.02 A in the N-N bond length may be distinguished using this approach.

218 The change of the inter-atomic bond length mechanism is argued to be the most plausible

219 pressure, as judged by enthalpy criteria and bond length metrics.

220 luctuations of backbone torsion angles and H-bond lengths, not by transient helix breaking.

221 o measure a 0.1 A displacement in the oxygen bond length occurring in a time interval of approximatel

222 e transient dimethyl amine radical has a N-C bond length of 1.45+/-0.02 angstrom and a C-N-C bond ang

223 a para-coupled phenoxyl radical, revealed a bond length of 1.6055(23) A for the C4-C4a bond.

224 e compound II derivative were an iron-oxygen bond length of 1.82 A and an iron-sulfur bond length of

225 ffraction reveals a uranium-terminal nitride bond length of 1.825(15) angstroms (where 15 is the stan

226 ne structure analysis found a short Fe-(O/N) bond length of 1.96 A at pH 8.50, strongly suggesting th

227 ws the shortest recorded Ce horizontal lineN bond length of 2.077(3) A.

228 gen bond length of 1.82 A and an iron-sulfur bond length of 2.24 A, both of which indicate an iron-ox

229 res a mu-eta(2):eta(2)-Se2 ligand with Se-Se bond length of 2.379(13) A.

230 possesses trans-planar geometry and an Al-Al bond length of 2.3943(16) A, which is the shortest dista

231 analysis also shows 24.2% (wt%) of FeS with bond length of 2.4 A in final nanohybrid.

232 The bond length of about 0.7 micrometers, comparable to the

233 to be 0.621 nm and is 4 times as long as the bond length of C-C backbone.

234 Furthermore, the average As-metal bond length of the KMnO(4) solids (R(As-Fe/Mn) = 3.24 +/

235 Thus, the Tb-Tb bond length of the single-electron bond is an exceedingl

236 but oxatriquinane has been found to have C-O bond lengths of 1.54 A.

237 degree of N1 protonation with the decreased bond lengths of 1.92, 1.55, and 1.28 A, respectively.

238 n this work with average Fe-Nimido and Fe-Fe bond lengths of 1.941(6) and 2.530(1) A, respectively.

239 ikely in an octahedral geometry with average bond lengths of 1.98 A.

240 ent interactions with Cu at their respective bond lengths of 2.1 and 2.3 A.

241 raction studies of AsP(3) have provided r(g) bond lengths of 2.3041(12) and 2.1949(28) A for the As-P

242 tion analysis reveals strongly elongated N-N bond lengths of dNN = 1.34(2)-1.35(3) A exceeding those

243 ds can reasonably reproduce the geometry and bond lengths of the active site.

244 Analysis of natural charges and bond lengths of the alkene-insertion transition state su

245 hile analysis of the differences between the bond lengths of the catalytic aspartates was performed u

246 ces of 0.010 +/- 0.008 A in the average Os-N bond lengths of the ground and excited states.

247 f complexes to be closely isostructural; the bond lengths of the Hf complex are slightly shorter, but

248 Typical bond lengths of the latter are 1.458 +/- 0.004, 1.385 +/

249 on of ultralong-range Rydberg molecules with bond lengths of ~100 nanometers and kilo-Debye permanent

250 ere are two types of Mo2O8 dimers with Mo-Mo bonds lengths of 2.22(2) and 2.28(2) A.

251 ical responses depending on number of double bonds, length of the acyl chain, infused lipid concentra

252 The very small difference in bond lengths, of ~0.06 A, means that it is impossible to

253 ivity of (19)F shielding to small changes in bond length, on the order of 0.01 angstrom or less, even

254 er bond lengths than their respective single bond lengths or their separations in (calculated) isolat

255 s, elongation of the copper-to-apical-oxygen bond length, or a beneficial crosstalk between a materia

256 lly due to surface roughness, unequal native bond lengths, or conditions that act to unzip the bonds.

257 observed trends had been proposed, based on bond lengths, pyramidalization angles, shape and energie

258 ing orbital also correlate strongly with O-P bond lengths (R = 0.88).

259 mid geometry is slightly distorted with Pb-O bond lengths ranging from 2.21 to 2.31 angstrom and O-Pb

260 lic complex features a relatively short Ni-M bond length, ranging from 2.3395(8) angstrom (Ni-Ga) to

261 ost distorted octahedra and a shortest Pb-Ru bond length relative to the average Pb-Ru bond length th

262 ucture of 7 reveals slightly longer U-O(oxo) bond lengths relative to 5.

263 iH2)[W(PMe3)3H2] possesses the shortest W-Si bond length reported.

264 d framework distortions that balance the C-O bond lengths required for covalency with host-guest dist

265 e triflates reveals 1.658 and 1.619 A C-O(+) bond lengths, respectively, the former of which is a new

266 Moreover, the calculated bond lengths reveal a reduction in bond-length alternati

267 and distance between amide units at chemical bond length-scale resolution.

268 ucture results from a 0.7% average Fe-ligand bond length shift between the 1 s and 2p core-ionized st

269 Si-O bond length shows first an increase due to the fourfold

270 ost [Fe(IV)(O)(TMC)(X)](+) species have Fe=O bond lengths similar to that of [Fe(IV)(O)(TMC)(NCMe)](2

271 are no relationships or correlations between bond lengths, strengths, and vibrational frequencies.

272 solid state, complexes 2-5 feature short U-E bond lengths, suggestive of actinide-ligand multiple bon

273 is species support mechanism I, and the Ni-C bond length suggests a homolytic cleavage of the Ni(III)

274 Examination of the carbon-nitrogen bond lengths suggests a degree of "partial protonation"

275 nes in these structures have somewhat longer bond lengths than their respective single bond lengths o

276 Ru bond length relative to the average Pb-Ru bond length that has ever been reported in a perovskite

277 Asp(17) has carboxylic acid bond lengths that are consistent with protonation, and w

278 The enol has bond lengths that are consistent with the expected bond

279 the neptunium atoms is evidenced by Np-O(yl) bond lengths that lie outside the typical range for Np(V

280 XeO3)4], in which the cage anions have Xe-Br bond lengths that range from 3.0838(3) to 3.3181(8) A.

281 Via direct charge transfer or by affecting bond lengths, the ligand effects cause the Pd d band to

282 re on the molecular scale, enabling the DNA "bond length" to be reversibly altered between 17 and 3 n

283 The inner icosahedron shows bond lengths typical for elemental gold while the distan

284 with the expected ca. 0.2 A increase in Fe-N bond length upon formation of the high-spin state.

285 these changes are associated with changes in bond lengths upon ionization; in general, better agreeme

286 means that it is impossible to obtain these bond lengths using Bragg diffraction in isolation.

287 e bond length <A-O> remains the same but the bond-length variance varies, we are able to demonstrate

288 atomic interfaces and capture Angstrom-level bond-length variations in single-layer graphene and MoS2

289 rees C, which is not in line with common C-C bond length versus bond strengths correlations.

290 eir exceptional properties to engineer their bond length, vibrational state, angular momentum and ori

291 pin crossover complexes are known to undergo bond length, volume, and enthalpy changes during spin tr

292 ct of the trans phosphine ligand on the Ir-C bond lengths was smaller than the effect of the substitu

293 comitant with the quadratic decrease in Ln-X bond lengths, was confirmed by reexamination of four oth

294 ular configuration, causing expansion of the bond length, which then returns back to the contracted v

295 ve region (cSAR, known earlier as qSAR), and bond lengths, which have been regressed against Hammett

296 r changes in the metal-oxo and metal-hydroxo bond lengths, which is traced to the difference in d-orb

297 gle of the carboxylate group and the C-CO(2) bond length with respect to the imidazolium ring is depe

298 Combining the variable bond length with their giant dipole moment of several hu

299 lts include the first measurement of an Am-S bond length, with a mean value of 2.921(9) A, by single-

300 The model explains an increased hydrogen bond length without nuclear quantum effects and for a pr