Introduction

Organic non-linear optical (NLO) materials during last two decades are subject of considerable research owing to their potential applications in optoelectronic technologies field for optical switching, signal processing, information storage and telecommunication [1, 2].

Organic compounds are widely focused as NLO materials due to their fabrication ease, low cost, facile synthesis and tailoring ability thus tuning their structure chemically according to desired properties of NLO [3]. Owing to recent developments in NLO field, second-order based NLO materials are finding practical applications due to combination of various synthetic strategies and their chemical tenability [4]. Intramolecular charge transfer (ICT) basically influences NLO material properties which originate mainly because of acceptor to donor moieties linked via π-conjugated bridge [5-8]. High performance NLO materials can be designed via modification of substituent’s properties such as acceptor, donor or π-conjugated bridge within acceptor-π-conjugated bridge- donor systems [9, 10].

Singer et al. in 1989 explored organic NLO molecule series with π-conjugation. They advocated property-structure relationship which affects β because of substituents, molecular configuration, π-conjugation system length and its type [11,12].

Janjua et al. in 2010 used quantum chemical methods for investigating halogen atoms effect on dipole polarizabilities and NLO second order response of hexa-molybdates derivatives like organoimido. It has been studied that NLO second order response of fluorine can be tuned due to its electron withdrawing ability [13]. Janjua et al. 2010 computed β value of terpyridine substituted hexamolybdates by studying halogens effect on NLO properties. The increase in computed β value is due to halogens incorporation (F, Br, I and Cl) in terpyridine ligand at the terminus [14].

An NLO response exhibit by organic compounds is often superior to those of pure inorganic materials [15,16]. Therefore, in this field organometallic compounds possessing NLO properties have opened new doors of achievement whereas search of new materials with greater NLO response are still in progress. Recently, POM-based inorganic-organic hybrid materials with large NLO properties have made great progress [17]. Janjua et al. concluded different results by studying electron withdrawing group effects on hexamolybdates and thus determined following aspects:

• The NLO second-order response can be enhanced remarkably via introducing electron acceptors at terpyridine-substituted hexamolybdates end which is attributed to increase in charge transfer between hexamolybdate and terpyridine.

• The large nonlinear second-order response is obtained via immediate introduction of CN and CF₃ at the terpyridine-substituted hexamolybdates end.

• The compounds containing CN and CF₃ exhibits larger second- order polarizabilities as compared to those having Cl and F.

• These compounds when electrons transition occurs to crucial excited states can turned to be an excellent 2-dimensional NLO candidates. It is due to off-diagonal second-order polarizability tensor (β _zyy) which originates via contribution of y polarized transition.

• One of advantageous features of acceptors is that they contributes in enhancement of NLO response by strengthening brigde conjugation [9].

For obtaining better nonlinear optical properties, LUMO-HOMO energy gap should be low. By increasing conjugation energy gap between LUMO and HOMO can be decreased. Another strategy used for lowering energy gap is structural modification. Similarly, more fluorine (F) atoms incorporation also results in decreasing LUMO-HUMO energy gap [18].

The NLO properties of acetylene derivatives (triphenylamine based α-cyanocinnamic acid) have been examined in this article. The author has designed triphenylamine based α-cyanocinnamic acid derivatives of acetylene via incorporation of fluorine (F) atom/atoms at phenyl ring of α-cyanocinnamic acid segment (see Fig. 1). Where, α-cyanoainnamic acid and triphenylamine act as acceptor (A) and donor (D) respectively. Effect of Fluorine atom on absorption and NLO properties has been tested by using density functional theory (DFT) and time-dependent density functional theory (TD-DFT) calculations. It is anticipated that obtained results may open a new gateway in providing useful mean for designing triphenylamine-α-cyanocinnamic acid segment based NLO compounds with tunable performance.

Computational details

Optimization of dyes structure in gas phase have been done via using B3LYP functional and 6-31+G* basis set [19]. Gaussian 09 program package was used for performing all calculations with the help of 10^-8 integration grid and convergence criteria (SCF 10^-8 au) [20]. However, frequency calculations have been performed for verification of optimized molecule’s nature [21,22]. Frequency analysis was performed to confirm that all structures in potential energy surfaces are present at local minima and there is no presence of imaginary frequency. Therefore, choosing appropriate functional absorption spectra of such organic dyes are calculated carefully. Coulomb-attenuating method CAMB3LYP functional, which is long-range corrected form of B3LYP, was used to calculate absorption spectra of dyes.[19] Success of this functional for determination of transition energies for a series of organic dyes is already proven.[23] The absorption spectra of the dyes were simulated by TD-DFT. Solvent effect (acetone) was undertaken using conductor-like polarizable continuum model (CPCM).[24]

Reproducible results of material’s optical properties are obtained using TDDFT/ DFT computational methods [25-29]. For studying acetone effect as solvent, CPCM (conductor-like polarizable continuum) model has been used [24]. Equation (1) [30] has been used for calculating average polarizability (α):

Ten hyperpolarizability (β _tot) components shown by Gaussian 09 program output file are as follows: β _xxx, β _xxy, β _xyy, β _yyy, β _xxz, β _xyz, β _yyz, β _xzz, β _yzz and β _zzz. Equation (2) represents the relation between these components and hyperpolarizability as under:

Molecular geometry

Substituted acetylene systems are used in this research. Two compounds such as α-cyanocinnamic acid and triphenylamine are used for substitution of acetylene. Fig. 1 shows the structures of these compounds D0-D4. Triphenylamine with formula (C₆H₅)₃N is an organic compound which as compared to most amines is non-basic in nature. Triphenylamine derivatives exhibit useful properties in electro-luminescence, electrical conductivity [31] and as hole-transporters in OLEDs [32].

Results and discussion

Effect of Fluorine (F) on LUMO and HOMO Energy Gap

LUMO and HOMO frontier molecular orbital’s determines molecular reactivity. Whereas, molecule’s chemical reactivity depends upon frontier energy gap as molecule becomes more polarizable with small energy gap. However, LUMO stabilization was higher which means LUMO energy decreased greatly as compared to HOMO. Hence, it results in lowering the energy gap between LUMO and HOMO. Table 1 shows calculated LUMO-HOMO energy gaps of D0-D4 are in following order; D4 < D1 < D0 < D3 < D2.

The energy gap of D3 and D2 systems is greater than D0 system whereas that of D4 and D1 is less than that of D0 system (the un-substituted system). Thus, D2 system is highly stabilized as compared to all other compounds. Largest energy gap is exhibited by D2 and smallest by D4. And with first fluorine substitution decrease in energy gap was observed. However, energy gap increases with second fluorine atom substitution and with third fluorine atom substitution, energy gap increases further. But remarkable decrease in energy gap is observed with subsequent substitution of fourth F atom.

Dipole Polarizability

Dipole polarizabilities are of important consideration for having better understanding of NLO second-order response (β). The average polarizability exhibits three major components i.e. α _zz, α _yy and α _xx. .Equation 3 is used for calculation of average polarizability (α ₀ ) and obtained results are shown by Table 2.

Table 2 shows components of dipole polarizability calculated for D0-D4. The (α_xx) component exhibits maximal value in studied compounds. That is why the property of studied compounds is determined dominantly via x-axis transition. Following formula is used for dipole polarizability along x-direction.

Where, in above equation α_xx relates directly to transition moment and inverse relation to transition energy. According to analysis of TDDFT, the generation of crucial excited state in D0-D4 occur along x-direction. Fig. 2 depicts frontier molecular orbitals.

Fig. 3 shows that D3 and D2 possess blue shift whereas D1 exhibits bathochromic shift and D4 system shows no change in the λ _max .

Static Second Order Polarizability.

Second-harmonic generation (SHG) is related to second-order polarizability. The static second-order polarizability (β _tot ) is defined as hyperpolarizability with zero-frequency and is therefore an estimate of molecular intrinsic hyperpolarizability in resonance effect. Individual components of D0-D4 and computed values of β _tot are given in Table 3. Owing to C1 symmetry, the second-order polarizability possesses ten components. It is evident from Table 3 that largest value is shown by β _xxx component in all studied compounds. Therefore, β _xxx component mainly contributes for second-order polarizability and major transfer of charge is along the x-direction. According to Table 3, it is clear that D0-D4 exhibit larger coefficients of second-order polarizability. For instance, the β _tot computed value for D4 is greater than average second-order polarizability of all D0-D3. Therefore, it indicates that except D3 and D2 all are showing excellent NLO second order response. Due to charge transfer from HOMO to LUMO the transition is assigned in system D3 and D2 (D-π-A configuration).

In D0-D4, due to CT along x-axis, the β _tot computed values indicate decrease in NLO response as follows: D4 > D1 > D0 > D3 > D2 whereas, calculated LUMO-HOMO energy gaps of D0-D4 are in following order; D4 < D1 < D0 < D3 < D2.

In D1 system, the β _xxx component is greater as compared to D0 system because of fluorine atom presence and D-A-A configuration establishment. β _xxx largest value is shown by D4 system. Among all five compounds, D4 system exhibits highest NLO response which is attributed to enhancement in α-cyanocinnamic acid donating ability (It is due to incorporation of four F atoms at outer side of benzene ring which in turns favors the conclusion that F atom substitution is important for enhancing the optical nonlinearity). According to Tables 1 and 4, it is interesting to note that a correlation exists between HOMO-LUMO gaps and β values; lower is the gap, higher is β.

In (D0-D4) studied compounds, demonstrating the structure-property relationship is mandatory to throw light for origin of NLO second-order properties. Through complex sum-over-states (SOS) expression, the two-state model has been established which linked between low-lying charge transfer transition and β [33]. The following model expression is applied for estimating β _CT in terms of static case.

Where,

E _gm , f _gm , and Δμgm represents transition energy, oscillator strength and dipole moment difference between the ground state (g) and the mth excited state (m), respectively.

The second-order polarizability in terms of two-state model expression resulted due to charge transfer (β _CT) is directly proportional to optical intensity whereas inversely related to transition energy in cubic form. Thus, in calculating β value for the studied compounds the decisive factor is low excitation energy. In terms of Table 4, the values of λ _gm for studied compounds are related with structural character. Increase in computed λ _gm values are shown as follows: D2 <D3 <D1 < D0 = D4.

The λ _gm value is larger for D1 and D3 whereas for D2 its value is only 374 nm and for D4 and D0 it increases a bit further i.e. upto 391 nm. By substituting electron withdrawing atom the absorption band shows bathochromic shift. The significant enhancement in β _tot value is observed because of this behavior as shown by Equation 4. Therefore, dominant contribution is attributed to excitation energy towards β _tot values of studied compounds. It has been demonstrated already that β value is directly proportional to Δμ (difference between excited and ground state dipole moment) and oscillator strength. However, it shows inverse relation towards transition energy. In D0-D4, for larger β value the low excitation energy is considered to be decisive factor for determining NLO response as given in Table 4. Thus, oscillator strength (f _gm) for D0-D4 systems is 1.538, 1.719, 1.595, 1.516 and 1.538, respectively. D4 and D0 systems exhibit same oscillating strength such that (1.583). In D0 system the excitation energy is higher than that of D4 system (which is a key factor in assigning NLO response in comparison of both compounds). Hence, in these systems the principle factor is low-lying excitation energy for increasing the value of β _tot . The strong oscillation strength is responsible for large β_tot values. In a nut shell, transition energy should be small but there are also some other factors which can influence NLO response including charge transfer and transition moments. Thus, following is the NLO response of D0-D4; D4 > D1 > D0 > D3 > D2

It is obvious that D4 system offers maximum β value via D-π-A configuration. It is also understandable that electron withdrawing substitution has a potential influence on NLO second-order property in our studied compounds. Thus, it can be concluded from these results that by incorporating electron withdrawing atom at benzene ring β value can be increased.

In D0-D4 another important factor is extension of π-conjugation via C≡C lengthening; and it also improved the delocalization. Generally, small energy difference is observed between charge transfer (CT) excited states (also enhances charge transfer degree accordingly) and ground states due to extended conjugation. It is well known that transition energy values governed NLO second-order property. Similarly, through introduction of an electron-withdrawing group (F) the LUMO-HOMO energy gap is decreased generally as in case of D4 and D1. However, D2 and D3 exhibit larger LUMO-HOMO energy gaps than D0. In terms of energy gaps of D0-D4, the D4 has least HOMO-LUMO energy gap value of 2.440.

Therefore, it is noticed that maximal NLO response is possessed by compound having smallest band gap (i.e. system D4 with band gap 2.440 eV). This band gap strongly influences the optical and electrical properties of material and is also a useful aspect of band structure. Generally, with increase in molecular size the band gap decreases. Transfer of electrons from one band to the other is done by means of recombination processes and carrier generation. Thus, due to generation of defect states within band gap via doping is useful in materials science for creating devices such as transistors, diodes, laser diodes, solar cells and others.

Conclusions

The α-cyanocinamic acids substituted with triphenylamine are found to possess considerably large static second-order polarizabilities. A compound having an electron acceptor (F) exhibits remarkably large second-order static polarizabilities. In terms of frontier MOs, the optical excitation analysis shows that the NLO response is attributed to charge transfer (CT) from triphenylamines to benzene ring with α-cyanocinamic acid. In D0-D4, CT along x-axis towards organic segment plays a key role in determining NLO response. According to the two-state model, the strong oscillation strength and the low excitation energy are the decisive factors in generating large β value. Compounds with longer wavelength transition possess higher computed β value. This research work reveals the NLO behavior of α-cyanocinamic acid-triphenylamine substituted compounds and therefore opens new doors for experimentalists in terms of designing NLO functional compounds with tunable performance. The present investigation provides an insight for NLO responses of triphenylamine substituted α-cyanocinamic acids and thus discloses the trend of NLO response. Our research presents vital confirmation for controlling the kinds of fluorinated rings that is a significant approach for the design of new appealing NLO compounds. This theoretical framework also highlights the NLO properties of organic dyes that can be valuable for their uses in modern hi-tech applications.

Acknowledgments

M.R.S.A. Janjua would like to acknowledge the support provided by the Deanship of Scientific Research (DSR) at King Fahd University of Petroleum & Minerals (KFUPM) for funding this work through project No. SR161009.

References

1. J.P. Costes, J.F. Lamere, C. Lepetit, P.G. Lacroix, F. Dahan, K. Nakatani, Synthesis, crystal structures, and nonlinear optical (NLO) properties of new Schiff-base nickel (II) complexes. Toward a new type of molecular switch?, Inorg. Chem. 44(6) (2005) 1973-1982.

2. S. Di Bella, I. Fragalà, Synthesis and second-order nonlinear optical properties of bis (salicylaldiminato) M (II) metalloorganic materials, Synth. Met. 115(1) (2000) 191-196.

3. D.J. Williams, Organic Polymeric and Non‐Polymeric Materials with Large Optical Nonlinearities, Angewandte Chemie International Edition in English 23(9) (1984) 690-703.

4. P. Günter, Nonlinear optical effects and materials, Springer 2012.

5. P.N. Prasad, D.J. Williams, Introduction to nonlinear optical effects in molecules and polymers, Wiley New York etc.1991.

6. D.S. Chemla, Nonlinear optical properties of organic molecules and crystals, Elsevier 2012.

7. M. Drozd, M. Marchewka, The structure, vibrational spectra and nonlinear optical properties of neutral melamine and singly, doubly and triply protonated melaminium cations-theoretical studies, J. Mol. Struct:Theochem 716(1) (2005) 175-192.

8. M.R.S.A. Janjua, Nonlinear optical response of a series of small molecules: quantum modification of π-spacer and acceptor, Journal of the Iranian Chemical Society (2017) 1-14.

9. M.R.S.A. Janjua, M. Amin, M. Ali, B. Bashir, M.U. Khan, M.A. Iqbal, W. Guan, L. Yan, Z.M. Su, A DFT Study on The Two‐Dimensional Second‐Order Nonlinear Optical (NLO) Response of Terpyridine‐Substituted Hexamolybdates: Physical Insight on 2D Inorganic-Organic Hybrid Functional Materials, Eur. J. Inorg. Chem. 2012(4) (2012) 705-711.

10. M.R.S.A. Janjua, M.U. Khan, B. Bashir, M.A. Iqbal, Y. Song, S.A.R. Naqvi, Z.A. Khan, Effect of π-conjugation spacer (C C) on the first hyperpolarizabilities of polymeric chain containing polyoxometalate cluster as a side-chain pendant: A DFT study, Comp. Theor. Chem. 994 (2012) 34-40.

11. K.D. Singer, J.E. Sohn, L. King, H. Gordon, H. Katz, C. Dirk, Second-order nonlinear-optical properties of donor-and acceptor-substituted aromatic compounds, JOSA B 6(7) (1989) 1339-1350.

12. J. Luo, M. Haller, H. Ma, S. Liu, T.-D. Kim, Y. Tian, B. Chen, S.-H. Jang, L.R. Dalton, A.K.-Y. Jen, Nanoscale architectural control and macromolecular engineering of nonlinear optical dendrimers and polymers for electro-optics, J. Phys. Chem. B 108(25) (2004) 8523-8530.

13. M.R.S.A. Janjua, Z.-M. Su, W. Guan, C.-G. Liu, L.-K. Yan, P. Song, G. Maheen, Tuning second-order non-linear (NLO) optical response of organoimido-substituted hexamolybdates through halogens: Quantum design of novel organic-inorganic hybrid NLO materials, Aust. J. Chem. 63(5) (2010) 836-844.

14. M.R.S.A. Janjua, W. Guan, L. Yan, Z.-M. Su, M. Ali, I.H. Bukhari, Prediction of robustly large molecular second-order nonlinear optical properties of terpyridine-substituted hexamolybdates: Structural modelling towards a rational entry to NLO materials, J. Mol. Graphics Modell. 28(8) (2010) 735-745.

15. M. Mutailipu, Z. Xie, X. Su, M. Zhang, Y. Wang, Z. Yang, M.R.S.A. Janjua, and S. Pan, Chemical Cosubstitution-Oriented Design of Rare-Earth Borates as Potential Ultraviolet Nonlinear Optical Materials, J. Am. Chem. Soc. 139 (2017) 18397−18405.

16. Y. Song, M. R. S. A. Janjua*, S. Jamil, M. Haroon, S. Nasir, Z. Nisar, A. Zafar, N. Nawaz, A. Batool, A. Aziz, The NLO properties of hybrid materials based on molybdate/hexamolybdate derivatives: A theoretical perspective for electro-optic modulation, Synth. Met. 198 (2014) 277-284.

17. M. Haroon, R. Mahmood, M.R.S.A. Janjua*, An Interesting Behavior and Nonlinear Optical (NLO) Response of Hexamolybdate Metal Cluster: Theoretical Insight into Electro-Optic Modulation of Hybrid Composites, J. Clust. Sci. 28 (2017) 2693-2708.

18. Y. Wu, W. Zhu, Organic sensitizers from D-π-A to D-A-π-A: effect of the internal electron-withdrawing units on molecular absorption, energy levels and photovoltaic performances, Chem. Soc. Rev. 42(5) (2013) 2039-2058.

19. T. Yanai, D. P. Tew, N. C. Handy, Chem. Phys. Lett. 2004, 393, 51-57.

20. S.P. Karna, Y. Zhang, M. Samoc, P. Prasad, B.A. Reinhardt, A.G. Dillard, Nonlinear optical properties of novel thiophene derivatives: Experimental and ab initio time‐dependent coupled perturbed Hartree-Fock studies, J. Chem. Phys. 99(12) (1993) 9984-9993.

21. J. Autschbach, Charge‐Transfer Excitations and Time‐Dependent Density Functional Theory: Problems and Some Proposed Solutions, Chemphyschem 10(11) (2009) 1757-1760.

22. A. Dreuw, M. Head-Gordon, Single-reference ab initio methods for the calculation of excited states of large molecules, Chem. Rev. 105(11) (2005) 4009-4037.

23. J. Zhang, H.-B. Li, Y. Wu, Y. Geng, Y.-A. Duan, Y. Liao, Z.-M. Su, Chem. J. Chinese U. 2011, 32, 1343-1348.

24. V. Barone, M. Cossi, J. Phys. Chem. A. 1998, 102, 1995-2001.

25. Preat, C. Michaux, D. Jacquemin, E.A. Perpete, Enhanced efficiency of organic dye-sensitized solar cells: triphenylamine derivatives, J. Phys. Chem. C 113(38) (2009) 16821-16833.

26. S. Kim, J.K. Lee, S.O. Kang, J. Ko, J.-H. Yum, S. Fantacci, F. De Angelis, D. Di Censo, M.K. Nazeeruddin, M. Grätzel, Molecular engineering of organic sensitizers for solar cell applications, J. Am. Chem. Soc. 128(51) (2006) 16701-16707.

27. D. Jacquemin, V. Wathelet, E.A. Perpete, C. Adamo, Extensive TD-DFT benchmark: singlet-excited states of organic molecules, J. Chem. Theory Comput. 5(9) (2009) 2420-2435.

28. M. Pastore, E. Mosconi, F. De Angelis, M. Grätzel, A computational investigation of organic dyes for dye-sensitized solar cells: benchmark, strategies, and open issues, J. Phys. Chem. C 114(15) (2010) 7205-7212.

29. A. Saylam, Z. Seferoglu, N. Ertan, Synthesis of new hetarylazoindole dyes from some 2-aminothiazole derivatives, Russ. J. Org. Chem. 44(4) (2008) 587-594.

30. A. Karakas, A. Elmali, H. Unver, Linear optical transmission measurements and computational study of linear polarizabilities, first hyperpolarizabilities of a dinuclear iron (III) complex, Spectrochim. Acta. A Mol. Biomol. Spectrosc. 68(3) (2007) 567-572.

31. Y.-J. Pu, M. Soma, H. Nishide, S. Shirai, J. Kido, Electroluminescence of poly (phenylenevinylene) s containing triphenylamine moieties in the main chain, Jpn. J. Appl. Phys. 41(1R) (2002) 362.

32. Z. Li, Z. Wu, W. Fu, P. Liu, B. Jiao, D. Wang, G. Zhou, X. Hou, Versatile fluorinated derivatives of triphenylamine as hole-transporters and blue-violet emitters in organic light-emitting devices, J. Phys. Chem. C 116(38) (2012) 20504-20512.

33. J.-L. Oudar, D. Chemla, Hyperpolarizabilities of the nitroanilines and their relations to the excited state dipole moment, J. Chem. Phys. 66(6) (1977) 2664-2668.

Author notes

* Corresponding author: e-mail: Janjua@kfupm.edu.sa/ <Phone: +966-550442019 >

IR