Artikelaktionen
Computational Chemistry
 Director: Univ.Prof. Peter R. Schreiner

Coworkers:
 Computational Chemistry

Current work:
Computational Chemistry: The fate of current methods and future challenges.
Stefan Grimme and Peter R. Schreiner Angew. Chem. Int. Ed. 2018, 57, xx–xx. Angew. Chem. 2018, 130, accepted for publication.
Polytriangulane. Wesley D. Allen,* Henrik Quanz, and Peter R. Schreiner*
J. Chem. Theory Comput. 2016, 12, 4707–4716. DOI: 10.1021/acs.jctc.6b00669The infinite spiroannelation of cyclopropanes in a nonbranched form will produce a σhelicene called polytriangulane, which is an unknown hydrocarbon with the formula C_{n}H_{n} comprised exclusively of formal C(sp^{3}) atoms. The structure of polytriangulane is elucidated here via a rigorous mathematical analysis of a C_{85}H_{88} prototype optimized by M062X/631G(d) density functional theory and an idealized polymer composed of equilateral cyclopropane units. The spiro carbons in polytriangulane form an exact, nonrepeating helix with a steep rise angle near 35°, a radius of only 0.41 Å, and irrational periodicity parameter very close to . A focal point analysis of the ring opening of cyclopropane to propene employing basis sets as large as ccpCV5Z and correlation treatments as extensive as CCSDT(Q) yields Δ_{f}H_{0}^{°}(cyclopropane) = 17.2 ± 0.1 kcal mol^{–1}. Subsequent application of CCSD(T)/CBS theory to a homodesmotic equation for ring aggregation predicts that Δ_{f}H_{0}^{°} = +16.1 kcal (mol CH)^{−1} for polytriangulane; hence, this compound is much more stable thermodynamically than acetylene. Similar computations on another hypothetical homodesmotic transformation indicate that the total strain energy in polytriangulane is 42.7 kcal per mole of cyclopropane units.
Heats of formation of platonic hydrocarbon cages by means of highlevel thermochemical procedures.
Amir Karton, Peter R. Schreiner and Jan M. L. Martin
J. Comput. Chem. 2016, 37, 49–58. DOI: 10.1002/jcc.23963Hydrocarbon cages are key reference materials for the validation and parameterization of computationally costeffective procedures such as density functional theory (DFT), semiempirical molecular orbital theory, and molecular mechanics. We obtain accurate total atomization energies (TAEs) and heats of formation (Δ_{f}H°_{298}) for platonic and prismatic hydrocarbon cages by means of the WnF12 explicitly correlated thermochemical protocols. We consider the following kinetically stable (CH)_{n} polycyclic hydrocarbon cages: (i) platonic hydrocarbons (tetrahedrane, cubane, and dodecahedrane), (ii) prismatic hydrocarbons (triprismane, cubane, and pentaprismane), and (iii) one truncated tetrahedrane (octahedrane). Our best theoretical heat of formation for cubane (144.8 kcal mol^{−1}) suggests that the experimental value adopted by the NIST thermochemical database (142.7 ± 1.2 kcal mol^{−1}) should be revised upwards by ∼2 kcal mol^{−1}. Our best heat of formation for dodecahedrane (20.2 kcal mol^{−1}) suggests that the semiexperimental value (22.4 ± 1 kcal mol^{−1}) should be revised downward by ∼2 kcal mol^{−1}. We use our benchmark WnF12 TAEs to evaluate the performance of a variety of computationally less demanding composite thermochemical procedures. These include the Gaussiann (Gn) and the complete basis set (CBS) methods. The CBSQB3 and CBSAPNO procedures show relatively poor performance with rootmeansquared deviations (RMSDs) of 4.2 and 2.5 kcal mol^{−1}, respectively. The best performers of the Gn procedures are G4 and G3(MP2)B3 (RMSD = 0.5 and 0.6 kcal mol^{−1}, respectively), while the worst performers are G3 and G4(MP2)6X (RMSD = 2.1 and 2.9 kcal mol^{−1}, respectively). Isodesmic and even homodesmotic reactions involving these species are surprisingly challenging targets for DFT computations.
Platonic hydrocarbons: Tetrahedrane (1, C_{4}H_{4}), cubane (2, C_{8}H_{8}), and dodecahedrane (3, C_{20}H_{20})
Nature Utilizes Unusual High London Dispersion Interactions for Compact Membranes Comprised of Molecular Ladders. J. Philipp Wagner and Peter R. Schreiner* J. Chem. Theory Comput. 2014, 10, 1353–1358. DOI: 10.1021/ct5000499
London dispersion interactions play a key role in nature, in particular, in membranes that constitute natural barriers. Here we demonstrate that the spatial alignment of “molecular ladders” ([n]ladderanes), i.e., highly unusual and strained alltransfused cyclobutane moieties, leads to much larger attractive dispersion interactions as compared to alkyl chains of the same length. This provides a rationale for the occurrence of peculiar ladderane fatty acids in the dense cell walls of anammox bacteria. Despite the energetic penalty paid for the assembly of such strained polycycles, the advantage lies in significantly higher, dispersiondominated interaction energies as compared to straightchain hydrocarbon moieties commonly found in fatty acids. We discern the dispersion contributions to the total interaction energies using a variety of computational methods including modern dispersioncorrected density functional theory and high level ab initio approaches. Utilizing larger assemblies, we also show that the intermolecular interactions behave additively.
Combined ab initio molecular dynamics and experimental studies show that carbon atom addition to benzene. Michael L. McKee,* HansPeter Reisenauer, and Peter R. Schreiner,* J. Phys. Chem. A. 2014, 118, in press. DOI: dx.doi.org/10.1021/jp501107b
Car–Parrinello molecular dynamics was used to explore the reactions between triplet and singlet carbon atoms with benzene. The computations reveal that, in the singlet C atom reaction, products are very exothermic where nearly every collision yields a product that is determined by the initial encounter geometry. The singlet C atom reaction does not follow the minimum energy path because the bimolecular reaction is controlled by dynamics (i.e., initial orientation of encounter). On the other hand, in a 10 K solid Ar matrix, ground state C(^{3}P) atoms do tend to follow RRKM kinetics. Thus, ab initio molecular dynamics (AIMD) results indicate that a significant fraction of C–H insertion occurs to form phenylcarbene whereas, in marked contrast to previous theoretical and experimental conclusions, the Ar matrix isolation studies indicate a large fraction of direct cycloheptatetraene formation, without the intermediacy of phenylcarbene. The AIMD calculations are more consistent with vaporized carbon atom experiments where labeling studies indicate the initial formation of phenylcarbene. This underlines that the availability of thermodynamic sinks can completely alter the observed reaction dynamics.
Polytwistane. Shiblee Barua, Henrik Quanz, Martin Olbrich, Peter R. Schreiner, Dirk Trauner, and Wesley D. Allen* Chem. Eur. J. 2014, 20, 1638–1645. DOI: 10.1002/chem.201303081.
Twistane, C_{10}H_{16}, is a classic D_{2}symmetric chiral hydrocarbon that has been studied for decades due to its fascinating stereochemical and thermodynamic properties. Here we propose and analyze in detail the contiguous linear extension of twistane with ethano (ethane1,2diyl) bridges to create a new chiral, C_{2}symmetric hydrocarbon nanotube called polytwistane. Polytwistane, (CH)_{n}, has the same molecular formula as polyacetylene but is composed purely of C(sp^{3})H units, all of which are chemically equivalent. The polytwistane nanotube has the smallest inner diameter (2.6 Å) of hydrocarbons considered to date. A rigorous topological analysis of idealized polytwistane and a C_{236}H_{242} prototype optimized by B3LYP density functional theory reveals that the polymer has a nonrepeating, alternating σhelix, with an irrational periodicity parameter and an instantaneous rise (or lead) angle near 15 °. A theoretical analysis utilizing homodesmotic equations and explicit computations as high as CCSD(T)/ccpVQZ yields the enthalpies of formation (twistane)=−1.7 kcal mol^{−1} and (polytwistane)= +1.28 kcal (mol CH)^{−1}, demonstrating that the hypothetical formation of polytwistane from acetylene is highly exothermic. Hence, polytwistane is synthetically viable both on thermodynamic grounds and also because no obvious pathways exist for its rearrangement to lowerlying isomers. The present analysis should facilitate the preparation and characterization of this new chiral hydrocarbon nanotube.
Steric crowding can stabilize a labile molecule: Solving the hexaphenylethane riddle. Stefan Grimme* and Peter R. Schreiner*
Angew. Chem. Int. Ed. 2011, 50, 12639–12642. Angew. Chem. 2011, 123, 12849–12853. Download Highlight: Nachr. Chem. 2012, 60, 108.
Abstract. 12 not so angry men: Hexaphenylethane is unstable, a phenomenon traditionally attributed to steric repulsion between the six phenyl rings. However, adding 12 bulky tertbutyl groups, one to each of the 12 meta positions, gives a stabile ethane derivative (see spacefilling model and potential energy curve for the dissociation of the central CC bond). This unexpected stabilization is shown to result from attractive dispersion interactions between the substituents.
σ/σ and π/πInteractions are Equally important: Multilayered Graphanes. Andrey A. Fokin,* Dennis Gerbig, and Peter R. Schreiner*
J. Am. Chem. Soc. 2011, 133, 20036–20039. Download
Abstract. The properties of singlesheet [n]graphanes, their doublelayered forms (diamondoids), and their van der Waals (vdW) complexes (multilayered [n]graphanes) were studied for n = 10–97 at the dispersioncorrected density functional theory (DFT) level utilizing B97D with a 631G(d,p) basis set; for comparison, we also computed a series of structures at M062X/631G(d,p) as well as B3LYPD3/631G(d,p) and evaluated SCSMP2/ccpVDZ singlepoint energies. The association energies for the vdW complexes reach 120 kcal mol^{–1} already at 2 nm particle size ([97]graphane dimer), and graphanes adopt layered structures similar to that of graphenes. The association energies of multilayered graphanes per carbon atom are rather similar and independent of the number of layers (ca. 1.2 kcal mol^{–1}). Graphanes show quantum confinement effects as the HOMO–LUMO gaps decrease from 8.2 eV for [10]graphane to 5.7 eV for [97]graphane, asymptotically approaching 5.4 eV previously obtained for bulk graphane. Similar trends were found for layered graphanes, where the differences in the electronic properties of doublesheet CH/σ vdW and doublelayered CC/σ diamondoids vanish at particles sizes of 1 nm. For comparison, we studied the parent CC/π systems, i.e., the single and doublesheet [n]graphenes (n = 10–130) for which the association energies demonstrate the same trends as in the case of [n]graphanes; in both cases the band gaps decrease with an increase in system size. The [112]graphene dimer (HOMO–LUMO gap = 0.5 eV) already approaches the 2D metallic properties of graphite.
Understanding the Torquoselectivity in 8πElectrocyclic Cascade Reactions: Synthesis of Fenestradienes versus Cyclooctatrienes. Catherine Hulot, Shadi Amiri,^{}Gaëlle Blond, Peter R. Schreiner, and Jean Suffert.
J. Am. Chem. Soc. 2009, 131, 13387. Download
Abstract. Unusual and novel polycyclic cyclooctatrienes, fenestradienes, and fenestrenes form readily from trienynes depending on the structure of the starting trienynes and the reaction conditions. The experimentally observed high torquoselectivities and complete diastereoselectivities of the 8πelectrocyclization products have been thoroughly studied using density functional computations at B3PW91/631g(d,p). The different P and Mhelical topologies for the Möbius aromatic transition structures are the origin of the observed torquoselectivities in the cyclooctatrienes. The Phelical topologies direct the newly formed single bonds into a favorable equatorial position of the neighboring cycloalkane moieties (X = ring size) that retain their most stable conformation. The Mhelical transition structures lead to an axial connection for the smaller rings (X = 4–6) and an equatorial connection for the seven and eightmembered cycloalkanes. This leads to unfavorable conformations for the larger cycloalkane moieties. Experiments and computations show that for trienynes involving small neighboring cycloalkane groups (X = 4–6) Mhelical topology is preferred toward cyclooctatrienes and in the following the corresponding fenestradienes can be formed as kinetic or even thermodynamic products; they convert to their more stable cyclooctatriene valence isomers derived from Phelical transition structures at higher temperatures. For larger cycloalkane moieties with more conformational flexibility only cyclooctatrienes with torquoselectivities derived from Phelical transition structures form.
NonKekulé NSubstituted mPhenylenes: NCentered Diradicals versus Zwitterions. Shadi Amiri, Peter R. Schreiner* J. Phys. Chem. 2009, 113, 11750–11757. Download
Abstract. The relationship between the structures and electronic ground state properties of nonKekulétype Nsubstituted mphenylenes was studied utilizing density functional theory (DFT), with the aim of determining the factors that lead to ground state triplet diradicals. At B3LYP/6311G(d,p)//B3LYP/6311G(d,p) we identified octahydropyridoquinoline with an exceptionally large singlet–triplet energy separation of +27.9 kcal mol^{–1}, in favor of the triplet. The highspin structures can readily be obtained by interruption of the full cyclic πdelocalization that avoids crossconjugation of the nitrogen radical centers. Introduction of additional heteroatoms on the other hand preferentially stabilizes the singlet zwitterionic resonance contributors in these systems. The identified diradicals show strong ferromagnetic exchange interactions between two radicalcenters.
3,5,7,9Substituted Hexaazaacridines: Toward Structures with Nearly Degenerate SingletTriplet Energy Separations. Peter Langer,* Shadi Amiri, Anja Bodtke, Nehad Saleh, Klaus Weisz, Halmar Görls, and Peter R. Schreiner*
J. Org. Chem. 2008, 73, 5048. Download
Abstract. Toward the goal of preparing stable, neutral openshell systems, we synthesized a novel series of pphenylsubstituted 3,5,7,9hexaazaacridine and 3,5,7,9hexaazaanthracene derivatives. The effects of substitution on the molecular electronic properties were probed both experimentally and computationally [B3LYP/6311G(d,p)//B3LYP/631G(d,p)]. While the experimentally prepared structures already have small (20–25 kcal/mol) singlettriplet energy gaps, systems with even smaller (<9 kcal/mol) singlettriplet energy separations can be realized through systematic variation of the substituent numbers, types, and patterns. Hexaazaanthracenes show generally smaller singlettriplet energy gaps than hexaazaacridines. Nitrogenbonded σ and πacceptor substituents that cause positive inductive and mesomeric effects as well as carbonbonded σdonor substituents make substituted hexaazaanthracenes promising candidates for purely organic highspin systems.