氫鍵復(fù)合物中鍵長變化與振動頻率移動相關(guān)性重訪

張 愚 馬 寧 王偉周

(洛陽師范學(xué)院化學(xué)化工學(xué)院,河南洛陽471022)

氫鍵復(fù)合物中鍵長變化與振動頻率移動相關(guān)性重訪

張 愚 馬 寧 王偉周*

(洛陽師范學(xué)院化學(xué)化工學(xué)院,河南洛陽471022)

X―H···Y(Y為電子供體)型氫鍵形成時,X―H鍵長伸長或縮短與相應(yīng)的X―H伸縮振動頻率紅移或藍(lán)移存在較強(qiáng)的相關(guān)性,這也是氫鍵光譜檢測和研究的基礎(chǔ).但是,最近的理論研究卻推翻了這一觀點,認(rèn)為X―H鍵長變化和相應(yīng)的X―H伸縮振動頻率移動在有些氫鍵體系中并不存在相關(guān)性(McDowell,S.A.C.; Buckingham,A.D.J.Am.Chem.Soc.2005,127,15515.).本文中,我們采用更為可信的計算方法,對這一問題進(jìn)行再研究.結(jié)果表明是錯誤的計算方法導(dǎo)致了McDowell和Buckingham得出錯誤的結(jié)論.在McDowell和Buckingham所研究的氫鍵體系中,X―H鍵長變化和相應(yīng)的X―H伸縮振動頻率移動仍存在較強(qiáng)的相關(guān)性.

氫鍵復(fù)合物;相關(guān);鍵長變化;振動頻率移動;密度泛函理論

1 Introduction

Hydrogen bond is one of the most important noncovalent interactions,which plays key roles in crystal engineering,supramolecular assembly,materials science,and biological system.1,2Infrared and Raman spectroscopies have played important roles in the detection of the hydrogen bonds:conventional X―H··· Y hydrogen bond is characterized by weakening of the X―H bond which causes elongation of this bond and a red shift of the X―H stretching frequency,and the blue-shifting X―H··· Y hydrogen bond is characterized by strengthening of the X―H bond which causes contraction of this bond and a blue shift of the X―H stretching frequency.3Obviously,the basis of the spectroscopic detection of the hydrogen bonds is that frequency shifts correlate very well with the bond-length changes and other characteristics of the hydrogen bond.3,4However,based on the ab initio computational results for a series of linear isoelectronic complexes of HCl with the proton acceptors N2,CO, or BF,McDowell and Buckingham5recently claimed that the widely believed correlation between the bond-length change and the frequency shift in the hydrogen-bonded complexes is unreliable.Such a conclusion is unusual,as it overturns the basis of the spectroscopic study of the hydrogen bond.We know now that the calculations of the bond-length change and the frequency shift are highly method-dependent.6Hence,it is reasonable to suppose that this conclusion may be a result of computational artifacts.In recent years,great progress has been made in the development of new quantum chemical methods.7-9It is the time to revisit this important issue by using more reliable computational methods.

The systems selected in the present study are the linear hydrogen-bonded complexes formed by HCl with N2,CO,BF,or CO2(Fig.1).All the complexes considered by McDowell and Buckingham are included here.For the halogen-bonded complexes,we found that,besides the computational method,the coupling between the X―Hal(Hal=Cl,Br,or I)stretching vibration and other vibrations and the anharmonicity of the X―Hal stretching vibration also have great influence on the bond-length change-frequency shift correlation.10For the hydrogen-bonded complexes,the effect of the coupling between the X―H stretching vibration and other vibrations on the bond-length change-frequency shift correlation can be neglected because of the small mass of the H atom.On the other hand, the study by Sándorfy11indicated that the effect of the anharmonicity of the X―H stretching vibration on the bond-length change-frequency shift correlation is also negligible in most cases.So we did not consider the effects of the vibrational coupling and the anharmonicity on the bond-length change-frequency shift correlation in this work.

Fig.1 Linear complexes considered in this workThe red dot lines represent the hydrogen bonds.

2 Computational details

Electronic structure calculations were carried out using the Gaussian 09 programs.12All the structures were fully optimized with“verytight”convergence criteria and characterized by frequency computations and wave function stability checks.Four newly developed density functionals,M05-2X,13,14M06-2X,14,15B2PLYP-D,16,17and mPW2PLYP-D,17,18were employed to investigate the correlation between bond-length change and vibrational frequency shift in hydrogen-bonded complexes.In order to examine the reliability of these density functionals,MP2, QCISD,and CCSD(T)calculations were also carried out.Both Pople?s basis sets and Dunning?s correlation-consistent series of basis sets with diffuse functions were used.The benchmark interaction energies in this work were calculated using the estimated CCSD(T)/CBS procedure,which can be found elsewhere.19An“ultrafine”integration grid(99 radial,590 angular points)was used for all the density functional theory(DFT)calculations to avoid the possible integration grid errors.The binding energies of the complexes were calculated using the supermolecule method.All binding energies are corrected for basis set superposition error(BSSE)using the counterpoise method of Boys and Bernardi.20

In the present study,the value of the bond-length change is given as the difference of the bond length between the complex and the monomer,so that a negative value of the bond-length change refers to a bond contraction and a positive value of the bond-length change indicates a bond elongation.Similarly,a negative value of the frequency shift refers to a red shift and a positive value of the frequency shift means a blue shift.

3 Results and discussion

3.1 Reliability of the M05-2X,M06-2X,B2PLYP-D, and mPW2PLYP-D density functionals

Fig.2 Potential energy curves for the linear complexCl―H···O≡C at different levels of theory All results reflect counterpoise correction.

Many newly developed density functionals have been prov-en to provide improved performance over conventional MP2 method for noncovalent interactions.7-9In this work,we used four popular density functionals M05-2X,M06-2X,B2PLYP-D,and mPW2PLYP-D for the calculations.The hybrid meta density functionals M05-2X and M06-2X are from Truhlar?s group and the double hybrid functionals B2PLYP-D and mPW2PLYP-D are from Grimme?s group.13-18In order to examine the reliability of these density functionals for the hydrogen-bonded complexes considered in the present study,we selected the linear complex Cl―H···O≡C as a model complex and calculated its potential energy curve at the M05-2X/ 6-311++G(3d,3p),M06-2X/6-311++G(3d,3p),B2PLYP-D/ 6-311++G(3d,3p),mPW2PLYP-D/6-311++G(3d,3p),MP2/ 6-311++G(2d,2p),QCISD/6-311++G(2d,2p),QCISD/6-311++ G(3df,3pd),and CCSD(T)/CBS levels of theory,respectively. The highly accurate CCSD(T)/CBS potential energy curve was used as our benchmark.As clearly shown in Fig.2,the MP2/ 6-311++G(2d,2p)and QCISD/6-311++G(2d,2p)calculations underestimate the binding energies and the mPW2PLYP-D/ 6-311++G(3d,3p)calculation tends to be overbound relative to the CCSD(T)/CBS benchmark.More important is the slope of the potential energy curve.It,in fact,determines how accurate the bond length and the vibrational frequency will be.If the two potential energy curves generated at the QCISD/6-311++ G(2d,2p)and QCISD/6-311++G(3df,3pd)levels of theory are removed from Fig.2,we can see that all the potential energy curves are almost in parallel with each other.Evidently,the slopes of the two potential energy curves generated at the QCISD/6-311++G(2d,2p)and QCISD/6-311++G(3df,3pd)levels of theory are inaccurate relative to the CCSD(T)/CBS benchmark,and furthermore they can not produce the correct results of the bond-length change and the frequency shift.Let us add here that McDowell and Buckingham?s conclusions are based on the QCISD/6-311++G(2d,2p)and QCISD/6-311++ G(3df,3pd)calculations.5In comparison with the CCSD(T)/ CBS benchmark,the similar slopes of the potential energy curves generated at the M05-2X/6-311++G(3d,3p),M06-2X/ 6-311++G(3d,3p),B2PLYP-D/6-311++G(3d,3p),and mPW2PLYP-D/6-311++G(3d,3p)levels of theory confirm the reliability of the density functionals M05-2X,M06-2X,B2PLYP-D,and mPW2PLYP-D for the study of the bond-length change-frequency shift correlation of the hydrogen-bonded complexes considered in the present study.

3.2 Selection of the basis set

The linear hydrogen-bonded complexes selected in the present study is very small,so it is possible to use very large basis set to eliminate the effect of the basis set superposition error and the basis set incompleteness error.However,considering the possible extension to large hydrogen-bonded complexes,it is meaningful to study the effect of the basis set on the bond length and the vibrational frequency here.

Table 1 lists the optimized geometries,Cl―H stretching frequencies and intensities,dipole moments,and BSSE-corrected binding energies of the studied complexes calculated at the M05-2X/6-311++G(d,p),M05-2X/6-311++G(3d,3p),and M05-2X/6-311++G(3df,3pd)levels of theory,respectively.Compar-ing the values in Table 1,it is found that the results calculated at the M05-2X/6-311++G(d,p)level of theory are obviously different from those calculated at the M05-2X/6-311++G(3d, 3p)and M05-2X/6-311++G(3df,3pd)levels of theory,for instance,the values of the Cl―H bond length calculated at the M05-2X/6-311++G(d,p)level of theory are all larger than the corresponding ones calculated at the M05-2X/6-311++G(3d, 3p)and M05-2X/6-311++G(3df,3pd)levels of theory,whereas the values of the Cl―H stretching frequency calculated at the M05-2X/6-311++G(d,p)level of theory are larger or smaller than the corresponding ones calculated at the M05-2X/6-311++ G(3d,3p)and M05-2X/6-311++G(3df,3pd)levels of theory;at the same time,it is also noticed that the results calculated at the M05-2X/6-311++G(3d,3p)level of theory are almost the same as those calculated at the M05-2X/6-311++G(3df,3pd) level of theory.These results indicate that the basis set 6-311++ G(3d,3p)yields converged results.In the following studies,we will use the basis set 6-311++G(3d,3p)for the calculations.

Table 1 Optimized geometries(r and R,in nm),Cl―H stretching frequencies(ν,in cm-1)and intensities(I,in km·mol-1),dipole moments(μ,in C·m),and BSSE-corrected binding energies(ΔECP,in kJ·mol-1)of the studied complexes calculated using M05-2X functional with basis sets 6-311++G(d,p),6-311++G(3d,3p),and 6-311++G(3df,3pd)

3.3 Cl―H bond-length change versus the Cl―H stretching frequency shift

The values of Cl―H bond-length change and the corresponding Cl―H stretching frequency shift upon the hydrogen-bonded complex formation are summarized in Table 2 and plots of the Cl―H bond-length change versus the corresponding Cl―H vibrational frequency shift are shown in Fig.3.

Fig.3 Correlation of Cl―H bond-length change with Cl―Hstretching frequency shift in hydrogen-bonded complexes

McDowell and Buckingham found,at their highest level of theory(QCISD/6-311++G(3df,3pd)),that blue shifts were obtained for Cl―H···F―B and Cl―H···O≡C,while red shifts were obtained for the other hydrogen-bonded complexes.5Surprisingly,a blue shift accompanied by a Cl―H bond elongation was also predicted for Cl―H···O≡C.5Here in Table 2, our results show that blue shift is obtained only for Cl―H···F―B,while Cl―H···O≡C and other complexes are all bound by the red shifting hydrogen bonds.At the same time,it can be seen from Table 2 that all the data are very normal,that is to say,the red shift is connected with the bond elongation and the blue shift is connected with the bond contraction.As mentioned above,it is the computational artifact that leads to the different results.Note that McDowell and Buckingham also calculated Cl―H···O≡C at the MP2/6-311++G(2d,2p)level of theory.Their MP2 results are in agreement with our results.This can be explained by the correct slope of the potential energy curve of MP2 calculations,as mentioned above.

The correlation between the bond-length change and the frequency shift for the Cl―H bond can be seen in Fig.3.Plots of the Cl―H bond-length change versus the corresponding vibrational frequency shift of the Cl―H stretch all give straight lines.The coefficient of determination of these linear fits(R2) is about 0.995 at the M05-2X/6-311++G(3d,3p)and M06-2X/ 6-311++G(3d,3p)levels of theory and about 0.999 at the B2PLYP-D/6-311++G(3d,3p)and mPW2PLYP-D/6-311++G(3d,3p) levels of theory.These results show that the correlation between the Cl―H bond-length change and the corresponding frequency shift is excellent in the hydrogen-bonded complexesstudied.

Table 2 Cl―H bond-length changes(Δr,in nm)and the corresponding Cl―H stretching frequency shifts(Δν,in cm-1)upon the hydrogen-bonded complexes formation,and the BSSE-corrected binding energies(ΔECP,in kJ·mol-1)of the studied complexes at various levels of theory

4 Conclusions

The Cl―H bond-length change and the corresponding vibrational frequency shift of the Cl―H stretch upon the hydrogen bond formation have been determined using high level ab initio and density functional theory computations.It is found that the bond-length change-frequency shift correlation is highly method-dependent.The computational artifacts can lead to false conclusions.Compared with the CCSD(T)benchmark, M05-2X,M06-2X,B2PLYP-D,and mPW2PLYP-D give reasonable results,whereas the wave function theory-based QCISD performs poorly.Employing more reliable M05-2X, M06-2X,B2PLYP-D,and mPW2PLYP-D calculations,we found that plots of the Cl―H bond-length change versus the corresponding vibrational frequency shift of the Cl―H stretch all give straight lines and the coefficients of determination of the fits are close to 1 in all cases,showing that the correlation between the Cl―H bond-length change and the corresponding frequency shift is excellent in the hydrogen-bonded complexes studied.The correlation also indicates that the red shift is connected with the bond elongation,whereas the blue shift is connected with the bond contraction,and vice versa.We believe that,in addition to the Cl―H bond studied here,the results for other X―H bonds should be the same.

The present study focuses only on the correlation between bond-length change and vibrational frequency shift of the hydrogen bond in the ground state.It is unclear whether the correlation still remains for the hydrogen bond in the electronically excited state.21Further study is underway in our laboratory.

(1) Desiraju,G.R.Angew.Chem.Int.Edit.2011,50,52.

(2) Arunan,E.;Desiraju,G.R.;Klein,R.A.;Sadlej,J.;Scheiner, S.;Alkorta,I.;Clary,D.C.;Crabtree,R.H.;Dannenberg,J.J.; Hobza,P.;Kjaergaard,H.G.;Legon,A.C.;Mennucci,B.; Nesbitt,D.J.Pure Appl.Chem.2011,83,1619.

(3) Hobza,P.;Havlas,Z.Chem.Rev.2000,100,4253.

(4) Li,X.;Liu,L.;Schlegel,H.B.J.Am.Chem.Soc.2002,124, 9639.

(5)McDowell,S.A.C.;Buckingham,A.D.J.Am.Chem.Soc. 2005,127,15515.

(6) Lu,P.;Lin,G.Q.;Li,J.C.J.Mol.Struct.-Theochem 2005,723, 95.

(7) Sun,T.;Wang,Y.B.Acta Phys.-Chim.Sin.2011,27,2553. [孫 濤,王一波.物理化學(xué)學(xué)報,2011,27,2553.]

(8) Schwabe,T.;Grimme,S.Accounts Chem.Res.2008,41,569.

(9) Sherrill,C.D.J.Chem.Phys.2010,132,110902.

(10) Wang,W.;Zhang,Y.;Ji,B.;Tian,A.J.Chem.Phys.2011,134, 224303.

(11) Sándorfy,C.J.Mol.Struct.2006,790,50.

(12) Frisch,M.J.;Trucks,G.W.;Schlegel,H.B.;et al.Gaussian 09, Revision C.01;Gaussian Inc.:Wallingford CT,2010.

(13) Zhao,Y.;Truhlar,D.G.J.Chem.Theory Comput.2006,2,1009.

(14) Zhao,Y.;Truhlar,D.G.Accounts Chem.Res.2008,41,157.

(15) Zhao,Y.;Truhlar,D.G.Theor.Chem.Acc.2008,120,215.

(16) Grimme,S.J.Chem.Phys.2006,124,034108.

(17) Schwabe,T.;Grimme,S.Phys.Chem.Chem.Phys.2007,9, 3397.

(18) Schwabe,T.;Grimme,S.Phys.Chem.Chem.Phys.2006,8, 4398.

(19) Pitoňák,M.;Janowski,T.;Neogrády,P.;Pulay,P.;Hobza,P. J.Chem.Theory Comput.2009,5,1761.

(20) Boys,S.F.;Bernardi,F.Mol.Phys.1970,19,553.

(21) Zhao,G.J.;Han,K.L.Accounts Chem.Res.doi:10.1021/ ar200135h.

November 4,2011;Revised:December 27,2011;Published on Web:December 30,2011.

Correlation between Bond-Length Change and Vibrational Frequency Shift in Hydrogen-Bonded Complexes Revisited

ZHANG Yu MA Ning WANG Wei-Zhou*
(College of Chemistry and Chemical Engineering,Luoyang Normal University,Luoyang 471022,Henan Province,P.R.China)

The correlation between the X―H bond-length change and the corresponding X―H stretching frequency shift upon X―H···Y(Y is an electron donor)hydrogen bond formation is the basis for the spectroscopic detection and investigation of the hydrogen bond.However,this view has been questioned in a recent report,suggesting that the widely accepted correlation between the bond-length change and the frequency shift in hydrogen-bonded complexes is unreliable(McDowell,S.A.C.;Buckingham,A.D.J.Am. Chem.Soc.2005,127,15515.).In this work,several robust computational methods have been used to investigate this issue.The results clearly show that a computational artifact leads to the conclusion incorrectly reported by McDowell and Buckingham and that the correlation between the X―H bond-length change and the corresponding X―H stretching frequency shift is still very good in the hydrogen-bonded complexes studied.

Hydrogen-bonded complex;Correlation;Bond-length change;Vibrational frequency shift; Density functional theory

10.3866/PKU.WHXB201112303

O641

?Corresponding author.Email:wzwanglab@yahoo.com;Tel:+86-379-65515113.

The project was supported by the National Natural Science Foundation of China(21173113),Aid Project for the Leading Young Teachers in Henan Provincial Institutions of Higher Education of China(2010GGJS-166),and Natural Science Foundation of Henan Educational Committee,China (2010A150017,2011B150024).

國家自然科學(xué)基金(21173113),河南省高等學(xué)校青年骨干教師資助計劃項目(2010GGJS-166)和河南省教育廳自然科學(xué)研究計劃項目(2010A150017,2011B150024)資助