ライフサイエンスコーパス: bond length

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

2 f freedom, increases with increasing valence bond length.

3 D, B3LYP consistently overestimates the C2-O bond length.

4 orrelation between protonation state and N-P bond length.

5 e structure with only minor perturbations in bond length.

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

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

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

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

10 er of hydrogen bonds having relatively short bond lengths.

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

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

13 delocalization interactions in impacting O-P bond lengths.

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

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

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

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

18 res with significantly different patterns of bond lengths.

19 t, having different directions and different bond lengths.

20 epsilon2...H...N (average R2= 0.98) hydrogen bond lengths.

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

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

23 The inequivalent O-C-O bond lengths [1.122 angstroms (A) for the O-C bond adjac

24 ferences between the C(1)-C(2) and C(2)-C(3) bond lengths, (13)delta(3)-(13)delta(1) values, and the

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

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

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

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

29 ects of oxygen lone pairs on the C-H and C-C bond lengths along the C-C-H coupling pathway.

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

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

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

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

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

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

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

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

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

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

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

41 ists between the hyperpolarizability and the bond length alternation.

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

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

44 43 nm spectral shift is due to an increased bond-length alternation of the protonated Schiff base of

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

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

47 Symmetry considerations, bond length alternations, and NICS values (a magnetic cr

48 In particular, the bond-length alternations across the vinylene bridging gr

49 These CC "bond lengths," among the longest ever reported, generall

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

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

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

53 und to decrease the unmodified thiolate Fe-S bond length and blue-shift the ligand-to-metal charge-tr

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

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

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

57 The combination of short bond length and high degree of pyramidization for the ce

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

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

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

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

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

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

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

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

66 pyridine reveals the expected differences in bond lengths and also a structural change from two copla

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

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

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

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

71 'strained' frameworks requiring unrealistic bond lengths and bond angles), and that an effective 'fi

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

73 mmetrical, allene structure with 1.336 A C=C bond lengths and considerable biradical character.

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

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

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

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

78 The bond lengths and other geometrical parameters such as po

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

80 Both the Nd-O bond lengths and the geometries about the oxo ions are r

81 3 calculations on 1a-c provided quantitative bond lengths and torsional angles to support the conclus

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

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

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

85 tropy is -173.9 to -177.2 ppm (for 1.02 A NH bond length) and the site-to-site CSA variability is +/-

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

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

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

89 is defined by the C(alpha)-C(alpha) virtual bond lengths, angles and dihedral angles, and the X-ray

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

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

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

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

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

95 culated incorporation energies and optimized bond lengths are presented.

96 or [2](2+), indicate geometries in which the bond lengths are shifted toward a quinoidal pattern rela

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

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

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

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

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

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

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

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

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

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

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

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

109 The change in the Tc-O bond length associated with the changes in temperatures

110 relation between increased atomic radius and bond length at C8 and decreased base pair stability.

111 ery well against CCSD, deviating in the C2-O bond length at most by 0.009 angstroms; it is, therefore

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

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

114 central two hydrogen atoms but also the H-H bond length between them depends significantly on the na

115 Bond lengths between pairs of atoms in covalent molecule

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

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

118 l model of such a triplex is consistent with bond length, bond angle, and energetic restrictions (sta

119 escribe its molecular geometry and to access bond lengths, bond angles, and a bowl depth.

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

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

122 on to the hydroquinone (H2Q) via the Pauling bond-length/bond-order paradigm.

123 51(10) A(2)) exhibits a shorter average Fe-O bond length but a much higher static Debye-Waller factor

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

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

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

127 studied, where B3LYP overestimates the C2-O bond length by 0.191 angstroms.

128 ide; on average, they overestimated the CCSD bond length by 0.2 angstroms.

129 s that the protonation state affects the N-P bond length by altering the magnitude of stabilizing n(O

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

131 exes with unconventionally long metal ligand bond lengths can be isolated that provide options to dev

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

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

134 Analysis reveals that Co2+-Se2- bond lengths change relatively little as the host is var

135 The H-Cl bond-length change and the harmonic vibrational frequenc

136 The widely believed correlation between the bond-length change and the sign of the frequency shift o

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

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

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

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

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

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

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

144 The disparate changes in bond length (DeltarCO << DeltarCN) are found to be conso

145 The N-P bond length depends on the overall protonation state whe

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

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

148 veals the origin of the observed metal-metal bond length disorder, distinctively different for each s

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

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

151 and characterize the cluster structures and bond length distributions using density functional theor

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

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

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

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

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

157 eometry and essentially bulklike metal-metal bond lengths, even for the smallest (few atom) nanoparti

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

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

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

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

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

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

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

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

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

167 rgy with respect to displacement of the H-Cl bond length from its equilibrium value in the isolated m

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

169 ol over a reaction taking place more than 20 bond lengths from the controlling centre, corresponding

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

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

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

173 to increased s-character and shorter carbene bond lengths (i.e., C-C, C-H).

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

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

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

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

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

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

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

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

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

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

184 between microscopic and average cation-anion bond lengths in Co2+-doped CdSe nanocrystals but not in

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

186 ional tight binding/molecular mechanics, the bond lengths in the concerted mechanism's transition sta

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

188 different cation positions and N2-H2...N7 H-bond lengths in the respective structures.

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

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

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

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

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

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

195 and the average first nearest-neighbor Pt-Pt bond length increases by 3%, agreeing well with experime

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

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

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

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

200 nd Co(2+)Cbi+ cofactors; however, the Co-OH2 bond length is lengthened by about 0.2 angstroms for the

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

202 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

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

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

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

206 ry shows the shortest alkyl carbon-copper(I) bond length known (1.8809 A) and a rather large H-C-H an

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

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

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

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

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

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

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

214 site in a Ni(micro(3)-S)(2)Fe face with mean bond lengths Ni-P = 2.147(9) A and Ni-S = 2.29(2) A.

215 The Cu-Se and Se-Cu bond lengths obtained from analysis of the Cu and Se K-E

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

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

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

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

220 X-ray diffraction revealed a Cr-Cr bond length of 1.8351(4) angstroms (where the number in

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

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

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

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

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

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

227 as one cyclic hydrogen bond N1...O6 with the bond length of 2.7 A.

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

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

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

231 ained from fits of the EXAFS region are Fe-O bond lengths of 1.78 A for the alkylperoxoiron(III) inte

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

233 CoO(2) structure, resulting in different M-O bond lengths of 1.93 and 2.07 Angstroms for Mn-O and Ni/

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

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

236 he Zr-(CH3)(bridging) and Al-(CH3)(bridging) bond lengths of 1b (2.505(4) A and 2.026(4) A, respectiv

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

238 ures the semibridging CO-ligand, with Fe-muC bond lengths of 2.15 and 1.85 A.

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

240 rgies, helical strain, dipole moments, and H-bond lengths of both types of helices, but especially fo

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

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

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

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

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

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

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

248 have a very early transition state, when the bond lengths of the reactants just began to change.

249 n 27 assumed a flat geometry (Figure 4); the bond lengths of the tetracycle in 27 also fit well into

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

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

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

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

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

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

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

257 The H-bond lengths r(OH) are 1.73 +/- 0.03 Angstrom and 1.60 +

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

259 a are highly distorted, with the interatomic bond lengths ranging from 1.690 to 1.847 A at 113 GPa.

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

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

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

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

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

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

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

267 Examination of bond lengths shows very limited variation, which argues

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

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

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

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

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

273 An analysis of the bond lengths suggests that a 17 atom delocalization path

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

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

276 ak slip bond were detected with an effective bond length that is characteristic of short-range, stiff

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

280 (S = 1/2), and, consistent with the extended bond length, the [FeO(2)](8) unit has only one Fe(III)-O

281 sing 17O chemical shift with increasing Si-O bond length, the shift observed also depends upon the ex

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

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

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

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

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

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

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

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

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

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

292 Unexpectedly, the Cu-Se bond lengths were found to undergo only minor changes du

293 Hydrogen-bond lengths were obtained from the nuclear quadrupolar

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