Calculation of band gaps in molecular crystals using hybrid functional theory

Transcription

1 Calculation of band gaps in molecular crystals using hybrid functional theory W. F. Perger Electrical Engineering and Physics Departments, Michigan Tech University, Houghton, MI Abstract Hybrid functional theory is applied for calculation of band gaps in the molecular crystals anthracene, pentaerythritol (PE), pentaerythritol tetranitrate (PETN), and cyclotrimethylene trinitramine (RDX). The B3LYP hybrid functional is observed to produce band gap estimates in reasonable agreement with experiment for anthracene and RDX. This approach, which has been successfully used recently for other materials, is efficient and practical, which is especially important for these large molecular crystals. Key words: molecular crystals, band gap PACS: Mb, Nc, At 1 Introduction Density-functional theory (DFT) in the local-density approximation (LDA) [1,2] and, more recently, the generalized gradient approximation [3] have been successful for calculating the total energy in molecules and solids. However, accurate band gap calculations for semiconductors and insulators remains a problem of contemporary interest [4]. The ability of DFT to provide accurate, ab initio, ground-state properties in molecules is well known, and in cases where correlation is not strong, it may be reasonable to treat solids and molecules in the same way [5], that is, with the same theoretical methods. Molecular crystals, such as those studied here, would seem to fall into this category. Encouraged by the recent work of Muscat, Wander, and Harrison [6] which showed that the hybrid functional approach of Becke [7] can be used to improve the agreement with experiment for calculated band gaps for a wide variety of materials, the same approach is applied here to the molecular crystals anthracene, pentaerythritol (PE), pentaerythritol tetranitrate (PETN), and cyclotrimethylene trinitramine (RDX). Molecular crystals have not been as Preprint submitted to Elsevier Science 20 November 2002

2 thoroughly investigated as other materials owing to the typical computational complexity involved. At the time of one of the first ab initio molecular crystal studies, on urea, just over ten years ago [8], a system with 30 atoms per unit cell was at the achievable limit. During the intervening years, the advances made in utilizing symmetry to improve performance of the Crystal program [9], the progress made in basis sets and correlation theory, especially at the molecular level, and the improvements in computer hardware, have made firstprinciples studies of relatively large molecular crystals possible. The purpose of this paper is to add to the growing body of knowledge on the use of DFT as a practical means of achieving accurate calculations for band gaps in materials, in this case the molecular crystals anthracene, PE, PETN and RDX. In addition to the relevance of the band gap as an important material property, the need for an accurate determination of the band gap assumes a special significance for the case of energetic materials such as RDX and PETN. In RDX, for example, a possible mechanism proposed by Gilman [10] for the shock-to-detonation transition is a strain-induced reduction of the band gap, ultimately leading to the breaking of the N NO 2 bond. Accurate band gap calculations are therefore of central importance for determining if reasonable wave front pressures could cause such a reduction in the band gap. For comparison, different model potentials and their effect on the band gaps and the molecular highest occupied molecular orbital (HOMO) - lowest unoccupied molecular orbital (LUMO) splitting will be presented. 2 Molecular crystals studied Anthracene, C 14 H 10, forms a monoclinic structure, space group P 2 1 /a with 2 molecules per unit cell. The internal (fractional) co-ordinates used in the current study for both the carbon and hydrogen atoms were taken from Cruickshank [11]. PE, C(CH 2 OH) 4, crystallizes in the tetragonal structure with space group I4. The internal co-ordinates were obtained from Eilerman and Rudman [12]. PETN, [C(CH 2 ONO 2 ) 4 ] is a molecular crystal with 29 atoms per molecule, with two molecules per unit cell, and belongs to the tetragonal P 42 1 c space group. The internal co-ordinates used were from Kitaigorodskii [13]. RDX, [(CH 2 NNO 2 ) 3 ] has 21 atoms per molecule, 8 molecules per unit cell, and belongs to the orthorhombic P bca space group, with internal coordinates from Choi and Prince [14]. This results in 1176 atomic orbitals for the 168 atoms per unit cell and for this size of a system, it becomes especially important to utilize efficient numerical techniques and accurate physical models in order to obtain results in a reasonable time-frame. This fact serves to motivate using practical computational approaches, such as the hybrid functional method, which was recently shown to provide good band gap estimates for semi-conductors, semi-ionic oxides, and transition metal oxides [6]. 2

3 3 Approach The Crystal98 [9] program was used, initially with a basis set of s(6)sp(2)sp(1) for carbon, nitrogen, and oxygen, and s(2)s(1) for hydrogen. A Gaussian basis set was chosen, a s(6)sp(2)sp(1) set for the carbon atom and a s(2)s(1) for the hydrogen atom ( 6-21g ), as it had been successfully used previously for RDX [15]. A slightly more complicated basis set was also tried, the optimized carbon basis set of Dovesi, et al. [8] and the effect this had on the band gap was observed; seeing little or no effect, the simpler basis set was chosen for the remainder of this work. The basis set superposition error (BSSE) was corrected via the counterpoise method, as previously done for urea [8]. In conjunction with this, a limited basis set optimization was performed by varying the scaling of the exponent of the outermost orbital, in a manner previously described for the molecular crystals RDX and TATB [15]. In that study, it was determined that the outermost exponent for hydrogen should be 1.05, and 1.10 for carbon, nitrogen, and oxygen. In the present study it was found for RDX that exponent values of 1.05 for hydrogen and 1.03 for C, N, and O resulted in the minimum energy; for anthracene, values of 1.0 for all atoms gave the lowest energy. However, in both cases, the differences in the total energy for these various exponent values were quite small, typically on the order of 0.1 to 0.01 a.u. Furthermore, a greater BSSE was found for larger exponent values. Therefore, the exponent scaling chosen for this study was 1.0 for all orbitals. Once the basis sets were determined, an efficient and practical means must be adopted for solving the Schrödinger equation while retaining the physics of exchange and correlation. In order to study the effect of the exchangecorrelation potential on the band gap, several potentials were chosen. The B3LYP functional was chosen based on its success to estimate band gaps for a variety of materials [6] and has the form: E xc = E LSDA xc + 0.2(E F ock xc Exc LSDA ) Exc GGA, (1) where LSDA is the local spin-density approximation and GGA is the generalized gradient approximation and the parameters were determined by Becke [7] to optimize atomization energies, ionization potentials, and proton affinities were several molecules. The B3LYP hybrid functional combines Becke s three-parameter functional [7] for the exchange with the non-local correlation potential of Lee-Yang-Parr [16]. The Crystal98 [9] program explicitly evaluates the non-local Fock energy, then blends 20% of that value into the hybrid functional, as shown in Eq. (1). A second hybrid functional used was the B3PW which uses the Becke exchange 3

4 combined with the Perdew-Wang GGA (PWGGA) [17 20] correlation. Next, a LDA exchange and von Barth-Hedin (VBH) [21] correlation potential (nonhybrid) functional was chosen. Finally, for comparison, a Hartree-Fock (HF) potential was used. 4 Results Figure 1 shows the total density of states (DOS) for anthracene using the simpler 6-21g basis set and Figure 2 shows the DOS using the B3LYP hybrid DFT functional. As can be seen by comparing those figures, the band gap narrows from about 8.2 to about 3.6 ev. The band structure for the upper 5 valence bands and lowest 5 conduction bands using the B3LYP potential is shown in Figure 3. As with the molecular crystal urea [8], some of the bands are rather flat, likely due to weak coupling of the crystalline environment on the molecular states. A comparison of the band gaps calculated for anthracene, PE, PETN, and RDX using the exchange-correlation functionals described earlier is given in Table 1. For comparison, the highest occupied molecular orbital (HOMO) - lowest unoccupied molecular orbital (LUMO) splittings are also given, as calculated both by using the Crystal98 and the Gaussian98 programs, where possible, using the same basis sets and model potentials. As is apparent from Table 1 Comparison of band gaps and HOMO-LUMO splittings in anthracene, PE, PETN and RDX for a variety of exchange and correlation potentials. All values are in ev and are at the k = (000)-point. Experimental values for the optical band gaps are 4.4eV for anthracene [22] and 3.4eV for RDX [23]. Potential Anthracene PE PETN RDX E gap HO-LU E gap HO-LU E gap HO-LU E gap HO-LU HF B3LYP B3PW LDA-VWN Table 1, the Hartree-Fock potential over-estimates the band gap relative to experiment by roughly a factor of 2 for anthracene and a factor of 4 for RDX, in agreement with previous work [5], whereas the LDA potential predicts a value which is roughly half of the experimental one, also in general agreement with previous observations [24]. A previous second-order perturbation theory calculation gave a band gap value of 5.25eV for RDX [25], in reasonable agreement with the B3LYP band gap of 5.54eV. 4

5 In summary, the results of this study for anthracene, PE, PETN, and RDX indicate the utility of the B3LYP hybrid functional as an efficient means for calculating band gaps for these molecular crystals, as had been recently observed in other materials [6]. Acknowledgements The author would like to acknowledge the financial support of the US Office of Naval Research (MURI program) for this work. Also acknowledged are the extended visits at and collaboration with the Institute for Shock Physics, Washington State University, where Dr. Y. Gupta, et al., provided the motivation for this work. Discussions with Dr. Ravi Pandey and Dr. Miguel Blanco are also gratefully acknowledged. 5

6 References [1] P. Hohenberg, W. Kohn, Phys. Rev. 136 (1964) B864. [2] W. Kohn, L. J. Sham, Phys. Rev. 140 (1965) A1133. [3] J. P. Perdew, K. Burke, Y. Wang, Phys. Rev. B. 54 (23) (1996) [4] I. N. Remediakis, E. Kaxiras, Phys. Rev. B. 59 (8) (1999) [5] P. Fulde, Electron Correlations in Molecules and Solids, Springer-Verlag, Berlin, [6] J. Muscat, A. Wander, N. M. Harrison, Chem. Phys. Lett. 342 (2001) [7] A. D. Becke, J. Chem. Phys. 98 (1993) [8] R. Dovesi, M. Causà, R. Orlando, C. Roetti, V. Saunders, J. Chemical Physics 92 (12) (1990) [9] V. R. Saunders, R. Dovesi, C. Roetti, M. Causà, N. M. Harrison, R. Orlando, C. M. Zicovich-Wilson, CRYSTAL98 User s Manual, University of Torino, Torino, [10] J. J. Gilman, Phil. Mag. B67 (1993) 207. [11] D. W. J. Cruickshank, Acta Cryst. 9 (1956) [12] D. Eilerman, R. Rudman, Acta Cryst. B35 (1979) [13] A. I. Kitaigorodskii, Organic Chemical Crystallography, Consultants Bureau Enterprises, New York, [14] C. S. Choi, Acta Cryst. B28 (1972) [15] A. B. Kunz, Phys. Rev. B. 53 (15) (1997) [16] C. Lee, W. Yang, R. G. Parr, Phys. Rev. B. 37 (1988) 785. [17] J. P. Perdew, Electronic Structure of Solids, Akademie Verlag, Berlin, [18] J. P. Perdew, Y. Wang, Phys. Rev. B. 23 (1981) [19] J. P. Perdew, Y. Wang, Phys. Rev. B. 40 (1989) [20] J. P. Perdew, K. Burke, Y. Wang, Phys. Rev. B. 45 (1992) [21] U. von Barth, L. Hedin, J. Phys. C: Solid State Phys 5 (1972) [22] P. J. Bounds, W. Siebrand, Chem. Phys. Letters 75 (1980) 414. [23] P. L. Marinkas, J. Lumin. 15 (1977) 57. [24] J. P. Perdew, M. Levy, Phys. Rev. Lett. 51 (1983) [25] M. M. Kuklja, A. B. Kunz, J. Appl. Phys. 89 (9) (2001)

7 1 Anthracene DOSS, Hartree-Fock 0.8 DOSS, arb. units Energy, in ev Fig. 1. Density of states for anthracene, using density-functional theory and the Hartree-Fock potential. 1 Anthracene DOSS, DFT-B3LYP 0.8 DOSS, arb. units Energy, in ev Fig. 2. Density of states for anthracene, using density-functional theory and the B3LYP hybrid functional. 7

8 Anthracene DFT-B3LYP (100) (000) (110) (100) 5 4 Energy, in ev (100) (000) (110) (100) Fig. 3. Band structure for anthracene, using density-functional theory and the B3LYP hybrid functional. 8