@article{GerlachMonningerSchleieretal.2021,
  author    = {Gerlach, Marius and Monninger, Sophie and Schleier, Domenik and Hemberger, Patrick and Goettel, James T. and Braunschweig, Holger and Fischer, Ingo},
  title     = {Photoelectron Photoion Coincidence Spectroscopy of NCl\(_{3}\) and NCl\(_{2}\)},
  series = {ChemPhysChem},
  volume    = {22},
  journal   = {ChemPhysChem},
  number    = {21},
  doi       = {10.1002/cphc.202100537},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-257322},
  pages     = {2164-2167},
  year      = {2021},
  abstract  = {We investigate NCl\(_{3}\) and the NCl\(_{2}\) radical by photoelectron-photoion coincidence spectroscopy using synchrotron radiation. The mass selected threshold photoelectron spectrum (ms-TPES) of NCl\(_{3}\) is broad and unstructured due to the large geometry change. An ionization energy of 9.7±0.1 eV is estimated from the spectrum and supported by computations. NCl2 is generated by photolysis at 213 nm from NCl\(_{3}\) and its ms-TPES shows an extended vibrational progression with a 90 meV spacing that is assigned to the symmetric N-Cl stretching mode in the cation. An adiabatic ionization energy of 9.94 ± 0.02 eV is determined.},
  language  = {en}
}
@article{WeiserCuiDewhurstetal.2023,
  author    = {Weiser, Jonas and Cui, Jingjing and Dewhurst, Rian D. and Braunschweig, Holger and Engels, Bernd and Fantuzzi, Felipe},
  title     = {Structure and bonding of proximity-enforced main-group dimers stabilized by a rigid naphthyridine diimine ligand},
  series = {Journal of Computational Chemistry},
  volume    = {44},
  journal   = {Journal of Computational Chemistry},
  number    = {3},
  doi       = {10.1002/jcc.26994},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-312586},
  pages     = {456 -- 467},
  year      = {2023},
  abstract  = {The development of ligands capable of effectively stabilizing highly reactive main-group species has led to the experimental realization of a variety of systems with fascinating properties. In this work, we computationally investigate the electronic, structural, energetic, and bonding features of proximity-enforced group 13-15 homodimers stabilized by a rigid expanded pincer ligand based on the 1,8-naphthyridine (napy) core. We show that the redox-active naphthyridine diimine (NDI) ligand enables a wide variety of structural motifs and element-element interaction modes, the latter ranging from isolated, element-centered lone pairs (e.g., E = Si, Ge) to cases where through-space π bonds (E = Pb), element-element multiple bonds (E = P, As) and biradical ground states (E = N) are observed. Our results hint at the feasibility of NDI-E2 species as viable synthetic targets, highlighting the versatility and potential applications of napy-based ligands in main-group chemistry.},
  language  = {en}
}
@article{AeschlimannBrixnerCinchettietal.2017,
  author    = {Aeschlimann, Martin and Brixner, Tobias and Cinchetti, Mirko and Frisch, Benjamin and Hecht, Bert and Hensen, Matthias and Huber, Bernhard and Kramer, Christian and Krauss, Enno and Loeber, Thomas H. and Pfeiffer, Walter and Piecuch, Martin and Thielen, Philip},
  title     = {Cavity-assisted ultrafast long-range periodic energy transfer between plasmonic nanoantennas},
  series = {Light: Science \& Applications},
  volume    = {6},
  journal   = {Light: Science \& Applications},
  doi       = {10.1038/lsa.2017.111},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-173265},
  year      = {2017},
  abstract  = {Radiationless energy transfer is at the core of diverse phenomena, such as light harvesting in photosynthesis\(^1\), energy-transfer-based microspectroscopies\(^2\), nanoscale quantum entanglement\(^3\) and photonic-mode hybridization\(^4\). Typically, the transfer is efficient only for separations that are much shorter than the diffraction limit. This hampers its application in optical communication and quantum information processing, which require spatially selective addressing. Here, we demonstrate highly efficient radiationless coherent energy transfer over a distance of twice the excitation wavelength by combining localized and delocalized\(^5\) plasmonic modes. Analogous to the Tavis-Cummings model, two whispering-gallery-mode antennas\(^6\) placed in the foci of an elliptical plasmonic cavity\(^7\) fabricated from single-crystal gold plates act as a pair of oscillators coupled to a common cavity mode. Time-resolved two-photon photoemission electron microscopy (TR 2P-PEEM) reveals an ultrafast long-range periodic energy transfer in accordance with the simulations. Our observations open perspectives for the optimization and tailoring of mesoscopic energy transfer and long-range quantum emitter coupling.},
  language  = {en}
}
@article{SaalfrankFantuzziKupferetal.2020,
  author    = {Saalfrank, Christian and Fantuzzi, Felipe and Kupfer, Thomas and Ritschel, Benedikt and Hammond, Kai and Krummenacher, Ivo and Bertermann, R{\"u}diger and Wirthensohn, Raphael and Finze, Maik and Schmid, Paul and Engel, Volker and Engels, Bernd and Braunschweig, Holger},
  title     = {cAAC-Stabilized 9,10-diboraanthracenes—Acenes with Open-Shell Singlet Biradical Ground States},
  series = {Angewandte Chemie International Edition},
  volume    = {59},
  journal   = {Angewandte Chemie International Edition},
  number    = {43},
  doi       = {10.1002/anie.202008206},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-217795},
  pages     = {19338 -- 19343},
  year      = {2020},
  abstract  = {Narrow HOMO-LUMO gaps and high charge-carrier mobilities make larger acenes potentially high-efficient materials for organic electronic applications. The performance of such molecules was shown to significantly increase with increasing number of fused benzene rings. Bulk quantities, however, can only be obtained reliably for acenes up to heptacene. Theoretically, (oligo)acenes and (poly)acenes are predicted to have open-shell singlet biradical and polyradical ground states, respectively, for which experimental evidence is still scarce. We have now been able to dramatically lower the HOMO-LUMO gap of acenes without the necessity of unfavorable elongation of their conjugated π system, by incorporating two boron atoms into the anthracene skeleton. Stabilizing the boron centers with cyclic (alkyl)(amino)carbenes gives neutral 9,10-diboraanthracenes, which are shown to feature disjointed, open-shell singlet biradical ground states.},
  language  = {en}
}
@article{KleinJoheWagneretal.2020,
  author    = {Klein, Philipp and Johe, Patrick and Wagner, Annika and Jung, Sascha and K{\"u}hlborn, Jonas and Barthels, Fabian and Tenzer, Stefan and Distler, Ute and Waigel, Waldemar and Engels, Bernd and Hellmich, Ute A. and Opatz, Till and Schirmeister, Tanja},
  title     = {New cysteine protease inhibitors: electrophilic (het)arenes and unexpected prodrug identification for the Trypanosoma protease rhodesain},
  series = {Molecules},
  volume    = {25},
  journal   = {Molecules},
  number    = {6},
  issn      = {1420-3049},
  doi       = {10.3390/molecules25061451},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-203380},
  year      = {2020},
  abstract  = {Electrophilic (het)arenes can undergo reactions with nucleophiles yielding π- or Meisenheimer (σ-) complexes or the products of the S\(_N\)Ar addition/elimination reactions. Such building blocks have only rarely been employed for the design of enzyme inhibitors. Herein, we demonstrate the combination of a peptidic recognition sequence with such electrophilic (het)arenes to generate highly active inhibitors of disease-relevant proteases. We further elucidate an unexpected mode of action for the trypanosomal protease rhodesain using NMR spectroscopy and mass spectrometry, enzyme kinetics and various types of simulations. After hydrolysis of an ester function in the recognition sequence of a weakly active prodrug inhibitor, the liberated carboxylic acid represents a highly potent inhibitor of rhodesain (K\(_i\) = 4.0 nM). The simulations indicate that, after the cleavage of the ester, the carboxylic acid leaves the active site and re-binds to the enzyme in an orientation that allows the formation of a very stable π-complex between the catalytic dyad (Cys-25/His-162) of rhodesain and the electrophilic aromatic moiety. The reversible inhibition mode results because the S\(_N\)Ar reaction, which is found in an alkaline solvent containing a low molecular weight thiol, is hindered within the enzyme due to the presence of the positively charged imidazolium ring of His-162. Comparisons between measured and calculated NMR shifts support this interpretation},
  language  = {en}
}
@article{KleinBarthelsJoheetal.2020,
  author    = {Klein, Philipp and Barthels, Fabian and Johe, Patrick and Wagner, Annika and Tenzer, Stefan and Distler, Ute and Le, Thien Anh and Schmid, Paul and Engel, Volker and Engels, Bernd and Hellmich, Ute A. and Opatz, Till and Schirmeister, Tanja},
  title     = {Naphthoquinones as covalent reversible inhibitors of cysteine proteases — studies on inhibition mechanism and kinetics},
  series = {Molecules},
  volume    = {25},
  journal   = {Molecules},
  number    = {9},
  issn      = {1420-3049},
  doi       = {10.3390/molecules25092064},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-203791},
  year      = {2020},
  abstract  = {The facile synthesis and detailed investigation of a class of highly potent protease inhibitors based on 1,4-naphthoquinones with a dipeptidic recognition motif (HN-l-Phe-l-Leu-OR) in the 2-position and an electron-withdrawing group (EWG) in the 3-position is presented. One of the compound representatives, namely the acid with EWG = CN and with R = H proved to be a highly potent rhodesain inhibitor with nanomolar affinity. The respective benzyl ester (R = Bn) was found to be hydrolyzed by the target enzyme itself yielding the free acid. Detailed kinetic and mass spectrometry studies revealed a reversible covalent binding mode. Theoretical calculations with different density functionals (DFT) as well as wavefunction-based approaches were performed to elucidate the mode of action.},
  language  = {en}
}
@article{PreitschopfSturmStroganovaetal.2023,
  author    = {Preitschopf, Tobias and Sturm, Floriane and Stroganova, Iuliia and Lemmens, Alexander K. and Rijs, Anouk M. and Fischer, Ingo},
  title     = {IR/UV Double Resonance Study of the 2-Phenylallyl Radical and its Pyrolysis Products},
  series = {Chemistry - A European Journal},
  volume    = {29},
  journal   = {Chemistry - A European Journal},
  number    = {13},
  doi       = {10.1002/chem.202202943},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-312338},
  year      = {2023},
  abstract  = {Isolated 2-phenylallyl radicals (2-PA), generated by pyrolysis from a nitrite precursor, have been investigated by IR/UV ion dip spectroscopy using free electron laser radiation. 2-PA is a resonance-stabilized radical that is considered to be involved in the formation of polycyclic aromatic hydrocarbons (PAH) in combustion, but also in interstellar space. The radical is identified based on its gas-phase IR spectrum. Furthermore, a number of bimolecular reaction products are identified, showing that the self-reaction as well as reactions with unimolecular decomposition products of 2-PA form several PAH efficiently. Possible mechanisms are discussed and the chemistry of 2-PA is compared with the one of the related 2-methylallyl and phenylpropargyl radicals.},
  language  = {en}
}
@phdthesis{Wehner2018,
  author    = {Wehner, Johannes},
  title     = {Wellenfunktionsbasierte Analyse zweidimensionaler Spektren: Wellenpaketbewegung in Dimeren und Quantendiffusionsdynamik},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-163555},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2018},
  abstract  = {Diese Arbeit befasst sich mit der st{\"o}rungstheoretischen Berechnung von zweidimensionalen Photonen-Echo-Spektren f{\"u}r das elektronische und vibronische Modell eines Homo- und Hetero-Dimers sowie f{\"u}r ein vibronisches Modell eines Monomers unter dem Einfluss einer System-Bad-Wechselwirkung. Bei der Analyse der Dimerspektren steht neben der Orientierungsmittelung der Polarisation dritter Ordnung der Unterschied zwischen elektronischen und vibronischen Spektren sowie der Vergleich der Spektren von Homo- und Hetero-Dimeren im Zentrum des Interesses. Bei der Analyse der Monomer-Spektren steht die Behandlung einer dissipativen Dynamik bzw. des vibrational-coolings innerhalb eines stochastischen Ansatzes im Vordergrund. Der erste Teil dieser Arbeit konzentriert sich auf die st{\"o}rungstheoretische Berechnung der Polarisation dritter Ordnung in Dimeren. Dabei werden alle Aspekte und Ergebnisse f{\"u}r verschiedene Geometrien der {\"U}bergangsdipolmomente analysiert und diskutiert. Die Berechnungen ber{\"u}cksichtigen dabei auch die zuf{\"a}llige Anordnung der Molek{\"u}le in der Probe. Die Zusammenh{\"a}nge zwischen den 2D-Spektren und den Eigenschaften der Monomereinheiten, die Abh{\"a}ngigkeit der Intensit{\"a}ten mancher Peaks von der zeitlichen Abfolge der Pulse sowie der Einfluss der elektronischen Kopplung und verschiedener {\"U}bergangsdipolmomente erm{\"o}glichen ein grundlegendes Verst{\"a}ndnis der elektronischen Photonen-Echo-Spektren. Im elektronischen Dimer wird der Hetero-Dimer-Charakter durch verschiedene Monomeranregungsenergien sowie unterschiedliche {\"U}bergangsdipolmomente der Monomereinheiten bestimmt. Der Einfluss dieser Gr{\"o}ßen auf die Photonen-Echo-Spektren kann durch die Kombination einer detaillierten analytischen Betrachtung und numerischen Rechnungen anschaulich nachvollzogen werden. In der vibronischen Betrachtungsweise zeigt sich, dass die Spektren deutlich an Komplexit{\"a}t gewinnen. Durch die Vibrationsfreiheitsgrade vervielfachen sich die m{\"o}glichen {\"U}berg{\"a}nge im System und damit die m{\"o}glichen Peakpositionen im Spektrum. Jeder Peak spaltet in eine Vibrationssubstruktur auf, die je nach ihrer energetischen Position mit anderen {\"u}berlagern kann. Der Vergleich zwischen Homo- und Hetero-Dimer-Spektren wird durch die Wahl verschiedener Vibrationsfrequenzen und unterschiedlicher Gleichgewichtsabst{\"a}nde entlang der Vibrationskoordinaten erweitert. Die Berechnung des Orientierungsmittels erfolgt mit zwei verschiedenen Ans{\"a}tzen. Zum einen wird das Mittel durch den numerischen sampling-Ansatz berechnet. Dabei werden Azimutal- und Polarwinkel in kleinen Winkelinkrementen abgetastet und f{\"u}r jede Kombination ein 2D-Spektrum berechnet. Die Einzelspektren werden anschließend gemittelt. Diese Methode erweist sich im Dimer als sehr effektiv. Zum anderen erlaubt die analytische Auswertung der Polarisation dritter Ordnung, das gemittelte Spektrum direkt in einer einzelnen Rechnung durch winkelgemittelte Gewichtungsfaktoren zu bestimmen. Bei der Berechnung der elektronischen 2D-Spektren ist diese Methode sehr leistungsf{\"a}hig, da alle Ausdr{\"u}cke analytisch bekannt sind. F{\"u}r vibronische Systeme ist dieser Ansatz ebenfalls sehr leistungsstark, ben{\"o}tigt aber eine einmalige aufwendige Analyse vor der Berechnung. Trotz der deutlich erh{\"o}hten Anzahl an Zustandsvektoren, die propagiert werden m{\"u}ssen, ist diese Methode circa zweimal schneller als die direkte Mittelung mit der sampling-Methode. Im zweiten Teil konzentriert sich die Arbeit auf die Beschreibung eines Monomers, das sich in einer dissipativen Umgebung befindet. Dabei wird auf die L{\"o}sung einer stochastischen Schr{\"o}dingergleichung zur{\"u}ckgegriffen. Speziell wird die sogenannte quantum-state-diffusion-Methode benutzt. Dabei werden nicht nur die Erwartungswerte f{\"u}r die Energie und den Ort, sondern auch die Polarisation dritter Ordnung - eine phasensensitive Gr{\"o}ße - bestimmt. In der theoretischen Fragestellung wird dabei, ausgehend von der von-Neumann Gleichung, die Zeitentwicklung der reduzierten Dichtematrix durch die Integration einer stochastischen zeitabh{\"a}ngigen Schr{\"o}dingergleichung reproduziert. In Rechnungen koppelt die Stochastik {\"u}ber die Erwartungswerte von Ort und Impuls die verschiedenen st{\"o}rungstheoretischen Korrekturen der Wellenfunktion miteinander. Die Spektren, die aus den numerischen Simulationen erhalten werden, spiegeln das dissipative Verhalten des Systems detailliert wider. Eine Analyse der Erwartungswerte von Ort und Energie zeigt, dass sich die einzelnen elektronischen Zust{\"a}nde wie ged{\"a}mpfte harmonische Oszillatoren verhalten und jeweils einen exponentiellen Zerfall abh{\"a}ngig von der Dissipationskonstante zeigen. Dieser Teil der Arbeit erweitert vorausgehende Untersuchungen, bei denen ein vereinfachter Ansatz zu Einsatz kam, der die korrelierte Stochastik nicht ber{\"u}cksichtigte.},
  subject      = {Molekulardynamik},
  language  = {de}
}
@phdthesis{Sauer2021,
  author    = {Sauer, Susanne},
  title     = {Implementation and Application of QM/MM Hybrid Methods},
  doi       = {10.25972/OPUS-24321},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-243213},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2021},
  abstract  = {Within this work, an additive and a subtractive QM/MM interface were implemented into CAST. The interactions between QM and MM system are described via electrostatic embedding. Link atoms are used to saturate dangling bonds originating from the separation of QM and MM system. Available energy evaluation methods to be combined include force fields (OPLSAA and AMBER), semi-empirical programs (Mopac and DFTB+), and quantum-chemical methods (from Gaussian, Orca, and Psi4). Both the additive and the subtractive interface can deal with periodic boundary conditions. The subtractive scheme was extended to enable QM/QM, three-layer, and multi-center calculations. Another feature only available within the subtractive interface is the microiteration procedure for local optimizations. The novel QM/MM methods were applied to the investigation of the reaction path for the complex formation between rhodesain and K11777. Benchmark calculations show a very good agreement with results from Gaussian-ONIOM. When comparing the relative energies obtained with different options to a computation where the whole system was treated with the "QM method" DFTB3, the electrostatic embedding scheme with option "delM3" gives the best results. "delM3" means that atoms with up to three bonds distance to the QM region are ignored when creating the external charges. This is done in order to avoid a double counting of Coulomb interactions between QM and MM system. The embedding scheme for the inner system in a three-layer calculation, however, does not have a significant influence on the energies. The same is true for the choice of the coupling scheme: Whether the additive or the subtractive QM/MM interface is applied does not alter the results significantly. The choice of the QM region, though, proved to be an important factor. As can be seen from the comparison of two QM systems of different size, bigger is not always better here. Instead, one has to make sure not to separate important (polar) interactions by the QM/MM border. After this benchmark study with singlepoint calculations, the various possibilities of CAST were used to approximate the solution of a remaining problem: The predicted reaction energy for the formation of the rhodesain-K11777 complex differs significantly depending on the starting point of the reaction path. The reason for this is assumed to be an inadequate adjustment of the environment during the scans, which leads to a better stabilization of the starting structure in comparison to the final structure. The first approach to improve this adjustment was performing the relaxed scan with a bigger QM region instead of the minimal QM system used before. While the paths starting from the covalent complex do not change significantly, those starting from the non-covalent complex become more exothermic, leading to a higher similarity of the two paths. Nevertheless, the difference of the reaction energy is still around 15 kcal/mol, which is far from a perfect agreement. For this reason, Umbrella Samplings were run. Here, the adjustment of the environment is not done by local optimizations like in the scans, but by MD simulations. This has the advantage that the system can cross barriers and reach different local minima. The relative free energies obtained by Umbrella Samplings with suitable QM regions are nearly identical, independently of the starting point of the calculation. Thus, \(\Delta A\) evaluated by these computations can be assumed to reproduce the real energy change best. An MD simulation that was started from the transition state in order to mimic a "real-time" reaction indicates a very fast adjustment of the environment during the formation of the complex. This confirms that Umbrella Sampling is probably better suitable to describe the reaction path than a scan, where the environment can never move strong enough to leave the current local minimum.},
  subject      = {Quantenmechanik},
  language  = {en}
}
@article{BruneckerMuessigArrowsmithetal.2020,
  author    = {Brunecker, Carina and M{\"u}ssig, Jonas H. and Arrowsmith, Merle and Fantuzzi, Felipe and Stoy, Andreas and B{\"o}hnke, Julian and Hofmann, Alexander and Bertermann, R{\"u}diger and Engels, Bernd and Braunschweig, Holger},
  title     = {Boranediyl- and Diborane(4)-1,2-diyl-Bridged Platinum A-Frame Complexes},
  series = {Chemistry - A European Journal},
  volume    = {26},
  journal   = {Chemistry - A European Journal},
  number    = {39},
  doi       = {10.1002/chem.202001168},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-214707},
  pages     = {8518 -- 8523},
  year      = {2020},
  abstract  = {Diplatinum A-frame complexes with a bridging (di)boron unit in the apex position were synthesized in a single step by the double oxidative addition of dihalo(di)borane precursors at a bis(diphosphine)-bridged Pt\(^{0}\)\(_{2}\) complex. While structurally analogous to well-known μ-borylene complexes, in which delocalized dative three-center-two-electron M-B-M bonding prevails, theoretical investigations into the nature of Pt-B bonding in these A-frame complexes show them to be rare dimetalla(di)boranes displaying two electron-sharing Pt-B σ-bonds. This is experimentally reflected in the low kinetic stability of these compounds, which are prone to loss of the (di)boron bridgehead unit.},
  language  = {en}
}