Jarosław Jan Panek

Dr. Jarosław Jan Panek

Faculty of Chemistry, University of Wroclaw, Wroclaw, Poland
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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18 March 2004 in Journal of the American Chemical Society
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Journal Article
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MSMarcin Stȩpień
Marcin Stȩpień
LLLechosław Latos-Grażyński
Lechosław Latos-Grażyński
LSLudmiła Szterenberg
Ludmiła Szterenberg
JPJarosław Jan Panek
Jarosław Jan Panek
ZLZdzisław Latajka
Zdzisław Latajka

29 May 2008 in Journal of the American Chemical Society
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Journal Article
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APAnca Pordea
Anca Pordea
MCMarc Creus
Marc Creus
JPJarosław Jan Panek
Jarosław Jan Panek
CDCarole Duboc
Carole Duboc
DMDéborah Mathis
Déborah Mathis
TWThomas R. Ward
Thomas R. Ward

28 May 2008 in Journal of Physical Organic Chemistry
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Journal Article
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MCMichał K. Cyrański
Michał K. Cyrański
AJAneta Jezierska
Aneta Jezierska
PKPaulina Klimentowska
Paulina Klimentowska
JPJarosław Jan Panek
Jarosław Jan Panek
ASAndrzej Sporzyński
Andrzej Sporzyński

29 January 2008 in The Journal of Physical Chemistry A
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Journal Article
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JSJernej Stare
Jernej Stare
JPJarosław Jan Panek
Jarosław Jan Panek
JEJuergen Eckert
Juergen Eckert
JGJože Grdadolnik
Jože Grdadolnik
JMJanez Mavri
Janez Mavri
DHDušan Hadži
Dušan Hadži

28 May 2007 in The Journal of Chemical Physics
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AJAneta Jezierska
Aneta Jezierska
JPJarosław Jan Panek
Jarosław Jan Panek
AKAleksander Koll
Aleksander Koll
JMJanez Mavri
Janez Mavri
Car-Parrinello molecular dynamics (CPMD) study was performed for an anharmonic system—an intramolecularly hydrogen bonded Mannich-base-type compound, 4,5-dimethyl-2(N,N-dimethylaminemethyl)phenol, to investigate the vibrational spectrum associated with the O–H stretching. Calculations were carried out for the solid state and for an isolated molecule. The classical CPMD simulation was performed and then the proton potential snapshots were extracted from the trajectory. The vibrational Schrödinger equation for the snapshots was solved numerically, and the (O–H) envelope was calculated as a superposition of the 0→1 transitions. The potential of mean force for the proton stretching mode was calculated from the proton vibrational eigenfunctions and eigenvalues incorporating statistical sampling, nuclear quantum effects, and effects of the environment. Perspectives for application of the presented methodology in the computational support of biocatalysis are given in the study.

27 July 2020 in RSC Advances
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SMSona Melikova
Sona Melikova
AVAlexander P. Voronin
Alexander P. Voronin
JPJarosław Jan Panek
Jarosław Jan Panek
NFNikita E. Frolov
Nikita E. Frolov
Anastasia V. ShishkinaAnastasia V. Shishkina
Anastasia V. Shishkina
MVMikhail Vener
Mikhail Vener
This paper bridges the gap between high-level ab initio computations of gas-phase models of 1 : 1 arene–arene complexes and calculations of the two-component (binary) organic crystals using atom–atom potentials. The studied crystals consist of electron-rich and electron-deficient compounds, which form infinite stacks (columns) of heterodimers. The sublimation enthalpy of crystals has been evaluated by DFT periodic calculations, while intermolecular interactions have been characterized by Bader analysis of the periodic electronic density. The consideration of aromatic compounds without a dipole moment makes it possible to reveal the contribution of quadrupole–quadrupole interactions to the π-stacking energy. These interactions are significant for heterodimers formed by arenes with more than 2 rings, with absolute values of the traceless quadrupole moment (Qzz) larger than 10 D Å. The further aggregation of neighboring stacks is due to the C–H⋯F interactions in arene/perfluoroarene crystals. In crystals consisting of arene and an electron-deficient compound such as pyromellitic dianhydride, aggregation occurs due to the C–H⋯O interactions. The C–H⋯F and C–H⋯O inter-stacking interactions make the main contribution to the sublimation enthalpy, which exceeds 150 kJ mol−1 for the two-component crystals formed by arenes with more than 2 rings.