Jacob Overgaard

Dr. Jacob Overgaard

Department of Chemistry, Aarhus Universitet, Aarhus, Denmark
orcid

Research Focus & Metrics

Academic Career Length

28Years (1999-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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21 December 2018 in Science
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PBPhilip C. Bunting
Philip C. Bunting
MAMihail Atanasov
Mihail Atanasov
EDEmil Damgaard-Møller
Emil Damgaard-Møller
MPMAURO PERFETTI
MAURO PERFETTI
ICIris Crassee
Iris Crassee
JLJeffrey R. Long
Jeffrey R. Long
Cobalt unfettered by its ligand field: Applied magnetic fields induce a field in any compound with unpaired electrons. However, for the induced field to persist once the applied field is gone, the electrons must be configured to manifest orbital angular momentum. Generally, the influence of ligands severely restricts that property in transition metal complexes. Bunting et al. now show that a cobalt ion is just barely affected by two linearly coordinated carbon ligands and, as such, exhibits maximal orbital angular momentum. Although its magnetic properties mainly pertain at very low temperature, its structure offers a more general design principle. Science , this issue p. eaat7319

14 August 2015 in IUCrJ
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VHVenkatesha R. Hathwar
Venkatesha R. Hathwar
MSMattia Sist
Mattia Sist
MJMads Ry Vogel Jørgensen
Mads Ry Vogel Jørgensen
AMAref H. Mamakhel
Aref H. Mamakhel
Xiaoping WangXiaoping Wang
Xiaoping Wang
BIBo Brummerstedt Iversen
Bo Brummerstedt Iversen
Rubrene is one of the most studied organic semiconductors to date due to its high charge carrier mobility which makes it a potentially applicable compound in modern electronic devices. Previous electronic device characterizations and first principles theoretical calculations assigned the semiconducting properties of rubrene to the presence of a large overlap of the extended π-conjugated core between molecules. We present here the electron density distribution in rubrene at 20 K and at 100 K obtained using a combination of high-resolution X-ray and neutron diffraction data. The topology of the electron density and energies of intermolecular interactions are studied quantitatively. Specifically, the presence of Cπ...Cπinteractions between neighbouring tetracene backbones of the rubrene molecules is experimentally confirmed from a topological analysis of the electron density, Non-Covalent Interaction (NCI) analysis and the calculated interaction energy of molecular dimers. A significant contribution to the lattice energy of the crystal is provided by H—H interactions. The electron density features of H—H bonding, and the interaction energy of molecular dimers connected by H—H interaction clearly demonstrate an importance of these weak interactions in the stabilization of the crystal structure. The quantitative nature of the intermolecular interactions is virtually unchanged between 20 K and 100 K suggesting that any changes in carrier transport at these low temperatures would have a different origin. The obtained experimental results are further supported by theoretical calculations.

19 May 2010 in Journal of the American Chemical Society
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DGDelphine Gauthier
Delphine Gauthier
ALAnders T. Lindhardt
Anders T. Lindhardt
EOEsben P. K. Olsen
Esben P. K. Olsen
Jacob OvergaardJacob Overgaard
Jacob Overgaard
TSTroels Skrydstrup
Troels Skrydstrup

15 December 2010 in The Journal of Physical Chemistry A
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James PlattsJames Platts
James Platts
Jacob OvergaardJacob Overgaard
Jacob Overgaard
Cameron JonesCameron Jones
Cameron Jones
BIBo B. Iversen
Bo B. Iversen
Andreas StaschAndreas Stasch
Andreas Stasch

12 February 2018 in Nature Materials
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HKHidetaka Kasai
Hidetaka Kasai
KTKasper Tolborg
Kasper Tolborg
MSMattia Sist
Mattia Sist
JZJiawei Zhang
Jiawei Zhang
VHVenkatesha R. Hathwar
Venkatesha R. Hathwar
BIBo B. Iversen
Bo B. Iversen

1 January 2018 in IUCrJ
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MFMalte Fugel
Malte Fugel
DJDylan Jayatilaka
Dylan Jayatilaka
EHEmanuel Hupf
Emanuel Hupf
Jacob OvergaardJacob Overgaard
Jacob Overgaard
VHVenkatesha R. Hathwar
Venkatesha R. Hathwar
SGSimon Grabowsky
Simon Grabowsky
Hirshfeld atom refinement (HAR) is a novel X-ray structure refinement technique that employs aspherical atomic scattering factors obtained from stockholder partitioning of a theoretically determined tailor-made static electron density. HAR overcomes many of the known limitations of independent atom modelling (IAM), such as too short element–hydrogen distances, r(X—H), or too large atomic displacement parameters (ADPs). This study probes the accuracy and precision of anisotropic hydrogen and non-hydrogen ADPs and of r(X—H) values obtained from HAR. These quantities are compared and found to agree with those obtained from (i) accurate neutron diffraction data measured at the same temperatures as the X-ray data and (ii) multipole modelling (MM), an established alternative method for interpreting X-ray diffraction data with the help of aspherical atomic scattering factors. Results are presented for three chemically different systems: the aromatic hydrocarbon rubrene (orthorhombic 5,6,11,12-tetraphenyltetracene), a co-crystal of zwitterionic betaine, imidazolium cations and picrate anions (BIPa), and the salt potassium hydrogen oxalate (KHOx). The non-hydrogen HAR-ADPs are as accurate and precise as the MM-ADPs. Both show excellent agreement with the neutron-based values and are superior to IAM-ADPs. The anisotropic hydrogen HAR-ADPs show a somewhat larger deviation from neutron-based values than the hydrogen SHADE-ADPs used in MM. Element–hydrogen bond lengths from HAR are in excellent agreement with those obtained from neutron diffraction experiments, although they are somewhat less precise. The residual density contour maps after HAR show fewer features than those after MM. Calculating the static electron density with the def2-TZVP basis set instead of the simpler def2-SVP one does not improve the refinement results significantly. All HARs were performed within the recently introduced HARt option implemented in the Olex2 program. They are easily launched inside its graphical user interface following a conventional IAM.