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Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table

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Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Zhao, Qing; Ng, Stanley S. H. and Kulik, Heather J. “Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table.” The Journal of Physical Chemistry C 120, no. 30 (August 2016): 17035– 17045 © 2016 American Chemical Society As Published http://dx.doi.org/10.1021/acs.jpcc.6b04361 Publisher American Chemical Society (ACS) Version Author's final manuscript Citable link http://hdl.handle.net/1721.1/109924 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. Page 1 of 45 The Journal of Physical Chemistry 1 2 3 4 5 6 7 Predicting the Stability of Fullerene Allotropes 8 9 10 11 12 Throughout the Periodic Table 13 14 15 16 1, 2 1 1, 17 Qing Zhao , Stanley S. H. Ng , and Heather J. Kulik * 18 19 20 1Department of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, MA 21 22 02139 23 24 2 25 Department of Mechanical Engineering, Massachusetts Institute of Technology, Cambridge, 26 27 MA 02139 28 29 30 We present a systematic study of the role of elemental identity in determining electronic, 31 energetic, and geometric properties of representative A28B28, A30B30, and A36B36 III-V (A=B, Al, 32 Ga, or In and B=N, P, or As) and II-VI (A=Zn or Cd and B=S or Se) fullerene allotropes. A 33 simple descriptor comprised of electronegativity differences and covalent radii captures the 34 relative fullerene stability with respect to a nanoparticle reference, and we demonstrate 35 transferability to group IV A (A=C, Si, or Ge) fullerenes. We identify the source of relative 36 72 37 stability of the four- and six-membered-ring-containing A36B36 and A28B28 fullerene allotropes to 38 the less stable, five-membered-ring containing A30B30 allotrope. Relative energies of hydrogen- 39 passivated single ring models explain why the even-membered ring structures are typically more 40 stable than the A30B30 fullerene, despite analogies to the well-known C60 allotrope. The ring 41 strain penalty in the four-membered ring is comparable to or smaller than the nonpolar bond 42 43 penalty in five-membered rings for some materials, and, more importantly, five-membered rings 44 are more numerous in A30B30 than four-membered rings in A36B36 or A28B28 allotropes. Overall, 45 we demonstrate a path forward for predicting the relative stability of fullerene allotropes and 46 isomers of arbitrary shape, size, and elemental composition. 47 48 49 50 51 52 53 54 55 56 57 58 59 1 60 ACS Paragon Plus Environment The Journal of Physical Chemistry Page 2 of 45 1 2 3 1. Introduction 4 5 6 7 Thirty years after the discovery of Buckminsterfullerene (C60) through vaporiZation of 8 9 graphite by laser irradiation1, the excellent properties and potential applications of this unusual 10 11 2 12 carbon allotrope continue to drive considerable scientific inquiry . Since their initial discovery, 13 3-6 14 C60 fullerenes have found broad technological relevance in polymer-fullerene solar cells , drug 15 16 7-8 9 delivery , and proposed hydrogen storage devices . The unusual shape and properties of C60 17 18 10 11 19 have motivated study of its formation mechanism both theoretically and experimentally . Soon 20 21 after the discovery of the carbon-based fullerene, isoelectronic boron nitride fullerenes were 22 23 synthesiZed by electron beam irradiation12 and later with more success through the arc-melting 24 25 13 14-15 15 15-17 15 26 method in a wide siZe range (BnNn, n=12 , 24 , 28 , 36 , and 48 ). These structures 27 28 differ from C60 in that they are proposed to only have even-membered rings with polar B-N 29 30 bonds, although transition metal dopants16-17 have also been observed to be present due to 31 32 33 synthesis conditions. We note that elemental boron, in particular, is well known to produce 34 35 unusual chemical bonding and allotropes18-19. Recently, hollow nanocage structures have been 36 37 20 21- 38 made from other elements, including an all boron fullerene and multilayered inorganic MoS2 39 24 21 40 and MoSe2 fullerene-like structures. 41 42 43 First-principles simulation can provide valuable insight into the relationship between the 44 45 46 unusual geometric structure and associated electronic properties for both fullerenes that have 47 48 been experimentally isolated and those that may yet still be synthesiZed. Of all of the binary 49 50 fullerenes, boron nitride structures have been the primary focus of numerous computational 51 52 25 26-33 53 semiempirical and density functional theory (DFT) studies, primarily at siZes 54 25-27, 29-32 26-27, 55 commensurate with experimentally characteriZed BN fullerenes , especially B36N36 56 57 29-31 28, 33 58 allotropes, or slightly larger structures . Simulations have estimated the 72-atom 59 2 60 ACS Paragon Plus Environment Page 3 of 45 The Journal of Physical Chemistry 1 2 3 fullerene to be most stable when 6 four-membered and 32 six-membered rings are present26, 4 5 28-29 6 although there has been some exploration of line defects, octagons, decagons and 7 8 dodecagons or with transition metal dopants30 and hydrogenated structures33. Beyond boron 9 10 11 nitride, there have been fewer studies of binary compounds comprised of other elements, and 12 34-46 13 typically the focus has been on III-V and II-VI binary AnBn fullerenes with light elements 14 15 (A=boron, aluminum, Zinc; B=nitrogen, phosphorus, oxygen, sulfur) and small siZe34-35, 38-47 16 17 45, 47-49 18 (n=12). There are a few exceptions in the literature with heavier elements (A=gallium, 19 36-37, 48-49 35 20 cadmium; B=arsenic) and larger siZes , and binary IV-IV Si12C12 and homogeneous 21 22 boron fullerenes50-51 have also been considered. One notable exception is a study by Beheshtian 23 24 34 25 and coworkers who focused on a broader view of the role that element substitution plays in 26 27 A12B12 (A=boron, aluminum; B=nitrogen, phosphorus) fullerene properties. In addition to 28 29 fundamental property studies, some investigations have focused on the potential of binary or 30 31 52-53 54-56 57 32 ternary III-V or II-VI fullerenes in nanotechnology as gas sensors, for drug delivery , or 33 34 as hydrogen storage materials58-62. 35 36 37 38 Despite numerous theoretical studies of structural, energetic, and electronic properties of III- 39 40 V and II-VI binary fullerenes, a thorough analysis of fullerenes throughout the periodic table has 41 42 not thus far been carried out in order to identify underlying chemical trends in stable fullerene 43 44 45 allotrope candidates. A better understanding of the element-specific rules that govern fullerene 46 47 allotrope stability will help accelerate identification of potentially synthetically accessible 48 49 candidates with novel materials properties. Here, we provide a comprehensive study of the 50 51 52 relative stability and properties of AnBn (n=28, 30, 36) fullerenes for 12 III-V materials 53 54 (A=B,Al,Ga, or In and B=N, P, or As), 4 II-VI materials (A=Zn or Cd and B=S or Se) with some 55 56 57 58 59 3 60 ACS Paragon Plus Environment The Journal of Physical Chemistry Page 4 of 45 1 2 3 comparison to unary IV C, Si, and Ge structures. In this study, we unearth simple, global 4 5 6 descriptors and structural models capable of predicting fullerene stabilities. 7 8 9 The outline of the paper is as follows. In Section 2, we present the Computational Details 10 11 12 of our study. Section 3 contains the Results and Discussion of the energetic and electronic 13 14 properties of stoichiometric III-V and II-VI A36B36 fullerenes along with comparisons and 15 16 evaluations of properties to A28B28 and A30B30 fullerenes. We provide our Conclusions in Section 17 18 19 4. 20 21 22 2. Computational Details 23 24 25 First-principles simulations. Calculations were carried out with the graphical-processing 26 27 63-64 65 28 unit (GPU)-accelerated quantum chemistry package, TeraChem . Geometry optimiZations 29 30 and band gap calculations were performed using DFT with the long-range corrected, hybrid 31 32 66 33 ωPBEh exchange-correlation functional (ω=0.2) and the composite LACVP* basis set. The 34 35 LACVP* basis set corresponds to an LANL2DZ effective core potential basis for the Zn, Cd, Ga, 36 37 In, As, and Se atoms and 6-31G* basis for the B, Al, N, P, and S atoms. 38 39 40 41 Structures. We used the B36N36 (B28N28) fullerene geometry obtained with the 42 67 43 CRYSTAL14 package as a starting point to generate all other A36B36 (A28B28) fullerenes. We 44 45 46 converted the B36N36 (B28N28) Cartesian coordinates to internal coordinates in the Gaussian Z- 47 48 matrix format, replaced boron or nitrogen atoms by A or B atoms, respectively, and initially 49 50 rescaled interatomic distances in the Z-matrix based on experimental A-B bond distances in AB 51 52 68 53 crystal structures . The optimal bond distances for the starting point of geometry optimiZations 54 55 of A36B36 fullerenes were obtained by scanning distances in 0.05 Å increments within ± 0.5 of 56 57 the experimental bond distances.
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