@phdthesis{Walter2015,
  author    = {Walter, Christof},
  title     = {Excitonic States and Optoelectronic Properties of Organic Semiconductors - A Quantum-Chemical Study Focusing on Merocyanines and Perylene-Based Dyes Including the Influence of the Environment},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-123494},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2015},
  abstract  = {The scope of computational chemistry can be broadened by developing new methods and more efficient algorithms. However, the evaluation of the applicability of the methods for the different fields of chemistry is equally important. In this thesis systems with an unusual and complex electronic structure, such as excitonic states in organic semiconductors, a boron-containing bipolaron and the excited states of pyracene were studied and the applicability of the toolkit of computational chemistry was investigated. Concerning the organic semiconductors the focus was laid on organic solar cells, which are one of the most promising technologies with regard to satisfying the world's need for cheap and environmentally sustainable energy. This is due to the low production and material costs and the possibility of using flexible and transparent devices. However, their efficiency does still not live up to the expectations. Especially the exciton diffusion lengths seem to be significantly too short. In order to arrive at improved modules, a fundamental understanding of the elementary processes occurring in the cell on the molecular and supramolecular level is needed. Computational chemistry can provide insight by separating the different effects and providing models for predictions and prescreenings. In this thesis, the focus was laid on the description of excitonic states in merocyanines and perylene-based dyes taking the influence of the environment into account. At first, the photochemical isomerization between two configurations of 6-nitro BIPS observed experimentally was studied by first benchmarking several functionals against SCS-ADC(2) in the gas phase and subsequently calculating the excited-state potential energy surface. The geometries obtained from a relaxed scan in the ground state as well as from a scan in the excited state were used. The environment was included using different polarizable continuum models. It was shown that the choice of the model and especially the question of the state specificity of the approach is of vital importance. Using the results of the calculations, a two-dimensional potential energy surface could be constructed that could be used to explain the experimental findings. Furthermore, the importance of the excited-state isomerization as a potential deactivation channel in the exciton transport was pointed out. Then the assessment of the suitability of different merocyanines for optoelectronic applications with quantum-chemical methods was discussed. At first, the effect of the environment on the geometry, especially on the bond length alternation pattern, was investigated. It was shown that the environment changes the character of the ground-state wave function of several merocyanines qualitatively, which means that the results of gas-phase calculations are meaningless - at least when a comparison with solution or device data is desired. It was demonstrated that using a polarizable continuum model with an effective epsilon, a qualitative agreement between the calculated geometry and the geometry in the crystal structure can be obtained. Therefore, by comparing the bond length alternation in solution and in the crystal, a rough estimate of the effect of the crystal environment can be made. It was further shown that the connection between the HOMO energy and the open-circuit voltage is not as simple as it is often implied in the literature. It was discussed that it is not clear whether the HOMO of a single molecule or a \$\pi\$-stack containing several monomers should be used and if the environmental charges of the bulk phase or the interface should be included. Investigating the dependence of the HOMO energy on the stack size yielded no definitive trend. Furthermore, it was discussed that the effect due the optimization of the modules (solvent, bulk heterojunction) during the production masks any potential correlation between the HOMO energy and measured open-circuit values. Therefore, a trend can only be expected for unoptimized bilayer cells. It was concluded that ultimately, the importance of the HOMO energy should not be overestimated. The correlation between the exciton reorganization energy and the so-called cyanine limit, which is predicted by a simple two-state model, was also discussed. By referring to the results of VB calculations, it was discussed that the correlation indeed exists and is non-negligible, although the effect is not as strong as one might have expected. In this context, a potential application of a VB/MM approach was covered briefly. The importance of the molecular reorganization energy and the device morphology was also discussed. It was concluded that the optimization of merocyanines for organic optoelectronic devices is inherently a multiparameter problem and one cannot expect to find one particular parameter, which solely controls the efficiency. The perylene-based dyes were studied with a focus on the description of a potential trapping mechanism involving an intermolecular motion in a dimer. The aim was to find methods which can be applied to larger model systems than a dimer and take the effect of the environment into account. As a test coordinate the longitudinal shift of two monomers against each other was used. At first, it was demonstrated how the character of an excited state in a dimer can be defined and how it can be extracted from a standard quantum-chemical calculation. Then several functionals were benchmarked and their applicability or failure was rationalized using the character analysis. Two recipes could be proposed, which were applied to a constraint optimization (only intermolecular degrees of freedom) in the excited states of the PBI dimer and to the description of the potential energy surfaces of ground and excited states along a longitudinal displacement in the perylene tetramer, respectively. It was further demonstrated that the semi-empirical OMx methods fail to give an accurate description of the excited-state potential energy surfaces as well as the ground-state surface along the test coordinate. This failure could be attributed to an underestimation of overlap-dependent terms. Consequently, it could be shown that the methods are applicable to large intermolecular distances, where the overlap is negligible. The results of DFT calculations with differently composed basis sets suggested that adding an additional single p-function for each atom should significantly improve the performance. QM/MM methods are ideally suited to take the effect of the environment on a a dimer model system into account. However, it was shown that standard force fields also give an incorrect description of the interaction between the monomers along the intermolecular coordinate. This failure was attributed to the isotropic atom-atom interaction in the repulsion term of the Lennard-Jones potential. This was corroborated using two simple proof-of-principle anisotropy models. Therefore, a novel force field called OPLS-AA_O was presented that is based on OPLS-AA, but uses an anisotropic model for the repulsion. The model involves the overlap integral between the molecular densities, which are modeled as a sum of atom-centered p-type Gaussian functions. It was shown that using this force field an excellent agreement with the DFT results can be obtained when the correct parameters are used. These parameters, however, are not very generalizable, which was attributed to the simplicity of the model in its current state (using the same exponential parameter for all atoms). As a short excursion, the applicability of an MO-based overlap model was discussed. It was demonstrated that the repulsion term based on the density overlap can be used to correct the failure of the OMx methods for the ground states. This is in accord with the assumption that an underestimation of the overlap terms is responsible for the failure. It was shown that OPLS-AA_O also gives an excellent description of the longitudinal shift in a PBI tetramer. Using the tetramer as a test system and applying the recipe obtained in the TDDFT benchmark for the QM-part and OPLS-AA_O for the MM-part in conjunction with an electrostatic embedding scheme, a QM/MM description of the excited states of the PBI dimer including the effect of the environment could be obtained. In the last chapter the theoretical description of the Bis(borolyl)thiophene dianion and the excited states of pyracene were discussed. The electronic structure of the Bis(borolyl)thiophene dianion - a negative bipolaron - was elucidated using DFT and CASPT2 methods. Furthermore, an estimation of the extent of triplet admixture to the ground state due to spin-orbit coupling was given. In the second project the S1 and S2 states of pyracene were computed using SCS-CC2 and SCS-ADC(2) and an estimation for the balance between aromaticity and ring strain was given. This also involved computing the vibrational frequencies in the excited states. In both studies the results of the computations were able to rationalize and complete experimental results.},
  subject      = {Exziton},
  language  = {en}
}
@phdthesis{Stehr2015,
  author    = {Stehr, Vera},
  title     = {Prediction of charge and energy transport in organic crystals with quantum chemical protocols employing the hopping model},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-114940},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2015},
  abstract  = {As organic semiconductors gain more importance for application, research into their properties has become necessary. This work investigated the exciton and charge transport properties of organic semiconducting crystals. Based on a hopping approach, protocols have been developed for the calculation of Charge mobilities and singlet exciton diffusion coefficients. The protocols do not require any input from experimental data except for the x-ray crystal structure, since all needed quantities can be taken from high-level quantum chemical calculations. Hence, they allow to predict the transport properties of yet unknown compounds for given packings, which is important for a rational design of new materials. Different thermally activated hopping models based on time-dependent perturbation theory were studied for the charge and exciton transport; i. e. the spectral overlap approach, the Marcus theory, and the Levich-Jortner theory. Their derivations were presented coherently in order to emphasize the different levels of approximations and their respective prerequisites. A short reference was made to the empirical Miller-Abrahams hopping rate. Rate equation approaches to calculate the stationary charge carrier mobilities and exciton diffusion coefficients have been developed, which are based on the master equation. The rate equation approach is faster and more efficient than the frequently used Monte Carlo method and, therefore, provides the possibility to study the anisotropy of the transport parameters and their three-dimensional representation in the crystal. The Marcus theory, originally derived for outer sphere electron transfer in solvents, had already been well established for charge transport in organic solids. It was shown that this theory fits even better for excitons than for charges compared with the experiment. The Levich-Jortner theory strongly overestimates the charge carrier mobilities and the results deviate even stronger from the experiment than those obtained with the Marcus theory. The latter contains larger approximations by treating all vibrational modes classically. The spectral overlap approach in combination with the developed rate equations leads to even quantitatively very good results for exciton diffusion lengths compared to experiment. This approach and the appendant rate equations have also been adapted to charge transport. The Einstein relation, which relates the diffusion coefficient with the mobility, is important for the rate equations, which have been developed here for transport in organic crystals. It has been argued that this relation does not hold in disordered organic materials. This was analyzed within the Framework of the Gaussian disorder model and the Miller-Abrahams hopping rate.},
  subject      = {Exziton},
  language  = {en}
}
@phdthesis{Schmidt2015,
  author    = {Schmidt, Thomas Christian},
  title     = {Theoretical Investigations on the Interactions of Small Compounds with their Molecular Environments},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-127860},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2015},
  abstract  = {Im ersten Teil dieser Arbeit wird eine Kombination theoretischer Methoden f{\"u}r die strukturbasierte Entwicklung neuer Wirkstoffe pr{\"a}sentiert. Ausgehend von der Kristallstruktur eines kovalenten Komplexes einer Modellverbindung mit dem Zielprotein wurde mit Hilfe von quantenmechanischen und QM/MM Rechnungen die genaue Geometrie des vorausgehenden nicht-kovalenten Komplexes betimmt. Letztere ist der bestimmende Faktor f{\"u}r die Reaktivit{\"a}t des Inhibitors gegen{\"u}ber der katalytisch aktiven Aminos{\"a}ure und damit f{\"u}r die Ausbildung einer kovalenten Bindung. Aus diesem Grund wurde diese Geometrie auch f{\"u}r die Optimierung der Substitutionsmusters des Ihnibitors verwendet, um dessen Affinit{\"a}t zum Zielenzyme zu verbessern ohne dass dieser seine F{\"a}higkeit kovalent an das aktive Zentrum zu binden verliert. Die Optimierung des Substitutionsmuster wurde doch Methode des Molekularen Dockings unterst{\"u}tzt, das diese optimal dazu geeignet sind, Bindungsaffinit{\"a}ten vorherzusagen, die durch eine Modifikation der chemischen Struktur entstehen. Eine Auswahl der besten Strukturen wurde anschließend verwendet, um zu {\"u}berpr{\"u}fen, ob die ver{\"a}nderten Molek{\"u}le noch gen{\"u}gen Reaktivit{\"a}t gegen{\"u}ber dem Zielprotein aufweisen. Molek{\"u}ldynamik Simulationen der neuen Verbindungen haben jedoch gezeigt, dass die ver{\"a}nderten Verbindungen nur so and das Protein binden, dass die Bilung eine kovalenten Bindung zum Enzym nicht mehr m{\"o}glich ist. Daher wurden in einem weiteren Schritt die Modellverbindungen weiter modifiziert. Neben {\"A}nderungen im Substitutionsmuster wurde auch die chemische Struktur im Kern ver{\"a}ndert. Die Bindungsaffinit{\"a}ten wurde wieder mittels Docking {\"u}berpr{\"u}ft. F{\"u}r die besten Bindungsposen wurden wieder Simulationen zur Molek{\"u}ldynamik durchgef{\"u}hrt, wobei diesmal die Ausbildung einer kovalenten Bindung zum Enzyme m{\"o}glich erscheint. In einer abschließenden Serie von QM/MM Rechnungen unter Ber{\"u}cksichtigung verschiedener Protonierungszust{\"a}nde des Inhibitors und des Proteins konnten Reaktionspfade und zugeh{\"o}rige Reaktionsenergien bestimmt werden. Die Ergebnisse lassen darauf schließen, dass eines der neu entwickelten Molek{\"u}le sowohl eine stark verbesserte Bindungsaffinit{\"a}t wie auch die M{\"o}glichkeit der kovalenten Bindung an Enzyme aufweist. Der zweite Teil der Arbeit konzentriert sich auf die Umgebungseinfl{\"u}sse auf die Elektronenverteilung eines Inhibitormodells. Als Grundlage dient ein vinylsulfon-basiertes Moek{\"u}l, f{\"u}r das eine experimentell bestimmte Kristallstruktur sowie ein theoretisch berechneter Protein Komplex verf{\"u}gbar sind. Ein Referendatensatz f{\"u}r diese Systeme wurde erstellt, indem der Konformationsraum des Inhibitors nach m{\"o}glichen Minimumsstrukturen abgesucht wurde, welche sp{\"a}ter mit den Geometrien des Molek{\"u}ls im Kristall und im Protein verglichen werden konnten. The Geometrie in der Kristallumgebung konnte direkt aus den experimentellen Daten {\"u}bernommen werden. Rechnungen zum nicht-kovalenten Protein Komplex hingegen haben gezeigt, dass f{\"u}r das Modellsystem mehrere Geometrien des Inhibiors sowie zwei Protonierungszust{\"a}nde f{\"u}r die katalytisch aktiven Aminos{\"a}uren m{\"o}glich sind. F{\"u}r die Analyse wurden daher alle m{\"o}glichen Proteinkomplexe mit der Kristallstruktur verglichen. Ebenso wurden Vergleiche mit der Geometrie des isolierten Molek{\"u}ls im Vakuum sowie der Geometrie in w{\"a}ssriger L{\"o}sung angestellt. F{\"u}r die Geometrie des Molek{\"u}ls an sich ergab sich eine gute {\"U}bereinstimmung f{\"u}r alle Modellsysteme, f{\"u}r die Wechselwirkungen mit der Umgebung jedoch nicht. Die Ausbildung von Dimeren in der Kristallumgebung hat einen stark stablisierenden Effekt und ist einer der Gr{\"u}nde, warum dieser Kristall so gut wie keine Fehlordungen aufweist. In den Proteinkomplexen hingegen ergibt sich eine Abstoßung zwischen dem Inhibitor und einer der katalytisch aktiven Aminos{\"a}uren. Als Ursache f{\"u}r diese Abstoßung konnte die Einf{\"u}hrung der Methylaminfunktion ausgemacht werden. Vermutlicherweise f{\"u}hrt diese strukturelle {\"A}nderung auch dazu, dass der Modellinhibitor nicht in der Lage ist, so wie die Leitstruktur K11777 an das aktive Zentrum des Enzyms zu binden.},
  subject      = {Theoretische Chemie},
  language  = {en}
}
@phdthesis{Lang2015,
  author    = {Lang, Melanie},
  title     = {Valence Shell Photoionization of Soot Precursors with Synchrotron Radiation},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-117038},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2015},
  abstract  = {A series of combustion relevant species like radicals, carbenes and polycyclic aromatic hydrocarbons were characterized in the gas phase by vacuum UV synchrotron radiation and their ionization energies (IE) and further spectroscopic details of the respective cations were retrieved from threshold photoelectron spectra. The reactive intermediates were generated by flash vacuum pyrolysis from stable precursor molecules. Furthermore three polycyclic aromatic hydrocarbons were investigated by threshold photoelectron spectroscopy, too. The experiment was performed at the VUV beamline of the Swiss Light Source in Villigen/Switzerland and the iPEPICO (imaging photoelectron photoion coincidence) setup was applied to correlate ions and electrons from the same ionization event. From the threshold photoelectron spectra and from quantum chemical computations the vibrational structure of the molecule cations and the geometry changes upon ionization were assigned. The ionization energies of the two C4H5 isomers 2-butyn-1-yl and 1-butyn-3-yl were assigned to 7.94±0.02 eV and 7.97±0.02 eV, respectively. The isomerization between the two isomers was computed to have a barrier of 2.20 eV, so a rearrangement between the two radicals cannot be excluded. From the threshold photoelectron spectra of the two constitutional C4H7 isomers 1-methylallyl and 2-methylallyl the ionization energies were assigned to 7.48±0.02 eV and to 7.59±0.02 eV for 1-E-methylallyl and 1-Z-methylallyl, as well as to 7.88±0.01 eV for 2-methylallyl. The two radicals 9-fluorenyl, C13H9, and benzhydryl, C13H11, were observed to ionize at 7.01±0.02 eV and 6.7 eV. The threshold photoelectron spectrum of benzhydryl also incorporated the signal of the diphenylmethyl carbene, C13H10, which has an IE at 6.8 eV. In addition, the head-to-head dimers of 9-fluorenyl and benzhydryl were observed as products in the pyrolysis. C26H18 has an IE at 7.69±0.04 eV and C26H22 has an IE at 8.13±0.04 eV. The three polycyclic aromatic hydrocarbon DHP (C14H16) 1-PEN (C18H22) and THCT (C22H16) were investigated in an effusive beam. The ionization energies were determined to IE(DHP)= 7.38±0.02 eV, IE(1-PEN)=7.58±0.05 eV and IE(THCT)=6.40±0.02 eV. Furthermore the thermal decomposition and the dissociative photoionization of diazomeldrum's acid was investigated. The pyrolysis products yielded beside several other products the two not yet (by photoelectron spectroscopy) characterized molecules E-formylketene, C3O2H2 and 2-diazoethenone, N2C2O. The dissociative photoionization showed the Wolff rearrangement to occur at higher internal energies.},
  subject      = {Ultraviolett-Photoelektronenspektroskopie},
  language  = {en}
}
@phdthesis{Holzmeier2015,
  author    = {Holzmeier, Fabian},
  title     = {Photoionization of Nitrogen-Containing Reactive Molecules with Synchrotron Radiation},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-127763},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2015},
  abstract  = {The photoionization of several nitrogen-containing reactive intermediates relevant in combustion processes was investigated in the gas phase employing VUV synchrotron radiation. The intermediates were either freshly prepared and stored under cryogenic temperatures during the experiment or generated in situ by vacuum flash pyrolysis of suitable precursor molecules. The iPEPICO (imaging photoelectron photoion coincidence) setups of the VUV beamlines at the Swiss Light Source and Synchrotron SOLEIL were then used to record mass-selected threshold photoelectron (TPE) spectra. TPE spectra reveal the ionization energy and vibrational structure in the cationic states can often be resolved, which enables to distinguish different isomers. Accurate ionization energies for the radicals carbonyl amidogen, pyrrolyl, and 3-picolyl, and for the closed shell molecules isocyanic acid and cyanovinylacetylene were obtained. The analysis of the dissociative photoionization of the pyrolysis precursors enables in some cases to retrieve thermochemical data. Beyond, the absolute photoionization cross section of the cyclic carbene cyclopropenylidene was determined, NEXAFS and normal Auger spectra of isocyanic acid were recorded and analyzed at the O1s, N1s, and C1s edges, and the dissociative photoionization and pyrolysis of 1,4-di-tert-butyl-1,4-azaborinine was studied.},
  subject      = {Dissoziative Photoionisation},
  language  = {en}
}
@phdthesis{Brunecker2015,
  author    = {Brunecker, Frank},
  title     = {Kohlenstoffnanorohr-Komplexe - Adsorption und Desorption von (Bio-)Polymeren},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-113485},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2015},
  abstract  = {Zur Charakterisierung der Wechselwirkungen zwischen organischen Dispergiermitteln und nanoskaligen Oberfl{\"a}chen stellen Komplexe aus Kohlenstoffnanor{\"o}hren und (Bio-)Polymeren aufgrund der großen Oberfl{\"a}che der Nanor{\"o}hren und der kommerziellen Verf{\"u}gbarkeit fluoreszenzmarkierter DNA-Oligomere unterschiedlicher L{\"a}nge sowie intrinsisch fluoreszierender Polymere ein vielversprechendes Modellsystem dar. Im Rahmen der vorliegenden Dissertation wurden verschiedene Methoden evaluiert, um die Stabilit{\"a}t derartiger Komplexe zu untersuchen und dadurch R{\"u}ckschl{\"u}sse auf das Adsorptionsverhalten der (Bio-)Polymere zu ziehen. Dabei konnte gezeigt werden, dass das publizierte helikale Adsorptionsmodell der DNA auf Kohlenstoffnanor{\"o}hren die Resultate der durchgef{\"u}hrten Experimente nur unzureichend beschreiben kann und stattdessen andere Adsorptionskonformationen in Erw{\"a}gung gezogen werden m{\"u}ssen.},
  subject      = {Kohlenstoff-Nanor{\"o}hre},
  language  = {de}
}
@phdthesis{Becker2015,
  author    = {Becker, Johannes},
  title     = {Development and implementation of new simulation possibilities in the CAST program package},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-132032},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2015},
  abstract  = {The aim of the present work is the development and implementation of new simulation possibilities for the CAST program package. Development included, among other things, the partial parallelization of the already existing force fields, extension of the treatment of electrostatic interactions and implementation of molecular dynamics and free energy algorithms. The most time consuming part of force field calculations is the evaluation of the nonbonded interactions. The calculation of these interactions has been parallelized and it could be shown to yield a significant speed up for multi-core calculations compared to the serial execution on only one CPU. For both, simple energy/gradient as well as molecular dynamics simulations the computational time could be significantly reduced. To further increase the performance of calculations employing a cutoff radius, a linkedcell algorithm was implemented which is able to build up the non-bonded interaction list up to 7 times faster than the original algorithm. To provide access to dynamic properties based on the natural time evolution of a system, a molecular dynamics code has been implemented. The MD implementation features two integration schemes for the equations of motion which are able to generate stable trajectories. The basic MD algorithm as described in Section 1.2 leads to the sampling in the microcanonical (NVE) ensemble. The practical use of NVE simulations is limited though because it does not correspond to any experimentally realistic situation. More realistic simulation conditions are found in the isothermal (NVT) and isothermalisobaric (NPT) ensembles. To generate those ensembles, temperature and pressure control has been implemented. The temperature can be controlled in two ways: by direct velocity scaling and by a Nose-Hoover thermostat which produces a real canonical ensemble. The pressure coupling is realized by implementation of a Berendsen barostat. The pressure coupling can be used for isotropic or anisotropic box dimensions with the restriction that the angles of the box need to be 90� . A crucial simulation parameter in MD simulations is the length of the timestep. The timestep is usually in the rang of 1fs. Increasing the timestep beyond 1fs can lead to unstable trajectories since the fastest motion in the system, usually the H-X stretch vibration can not be sampled anymore. A way to allow for bigger timesteps is the use of a constraint algorithm which constrains the H-X bonds to the equilibrium distance. For this the RATTLE algorithm has been implemented in the CAST program. The velocity Verlet algorithm in combination with the RATTLE algorithm has been shown to yield stable trajectories for an arbitrary length of simulation time. In a first application the MD implementation is used in conjunction with the MOPAC interface for the investigation of PBI sidechains and their rigidity. The theoretical investigations show a nice agreement with experimentally obtained results. Based on the MD techniques two algorithms for the determination of free energy differences have been implemented. The umbrella sampling algorithm can be used to determine the free energy change along a reaction coordinate based on distances or dihedral angles. The implementation was tested on the stretching of a deca-L-alanine and the rotation barrier of butane in vacuum. The results are in nearly perfect agreement with literature values. For the FEP implementation calculations were performed for a zero-sum transformation of ethane in explicit solvent, the charging of a sodium ion in explicit solvent and the transformations of a tripeptide in explicit solvent. All results are in agreement with benchmark calculations of the NAMD program as well as literature values. The FEP formalism was then applied to determine the relative binding free energies between two inhibitors in an inhibitor-protein complex. Next to force fields, ab-initio methods can be used for simulations and global optimizations. Since the performance of such methods is usually significantly poorer than force field applications, the use for global optimizations is limited. Nevertheless significant progress has been made by porting these codes to GPUs. In order to make use of these developments a MPI interface has been implemented into CAST for communication with the DFT code TeraChem. The CAST/TeraChem combination has been tested on the \$H_2 O_{10}\$ cluster as well as the polypeptide met-Enkephalin. The pure ab-initio calculations showed a superior behavior compared to the standard procedure where the force field results are usually refined using quantum chemical methods.},
  subject      = {Molekulardynamik},
  language  = {en}
}