Core electron chemical shifts of hydrogen-bonded structures

2009 ◽  
Vol 468 (4-6) ◽  
pp. 294-298 ◽  
Author(s):  
Guangde Tu ◽  
Yaoquan Tu ◽  
Olav Vahtras ◽  
Hans Ågren
2000 ◽  
Vol 122 (51) ◽  
pp. 12878-12879 ◽  
Author(s):  
Parwin Schah-Mohammedi ◽  
Ilja G. Shenderovich ◽  
Carsten Detering ◽  
Hans-Heinrich Limbach ◽  
Peter M. Tolstoy ◽  
...  

2011 ◽  
Vol 133 (9) ◽  
pp. 3120-3130 ◽  
Author(s):  
Niklas Ottosson ◽  
Knut J. Børve ◽  
Daniel Spångberg ◽  
Henrik Bergersen ◽  
Leif J. Sæthre ◽  
...  

2022 ◽  
Vol 13 (1) ◽  
Author(s):  
D. Mayer ◽  
F. Lever ◽  
D. Picconi ◽  
J. Metje ◽  
S. Alisauskas ◽  
...  

AbstractThe conversion of photon energy into other energetic forms in molecules is accompanied by charge moving on ultrafast timescales. We directly observe the charge motion at a specific site in an electronically excited molecule using time-resolved x-ray photoelectron spectroscopy (TR-XPS). We extend the concept of static chemical shift from conventional XPS by the excited-state chemical shift (ESCS), which is connected to the charge in the framework of a potential model. This allows us to invert TR-XPS spectra to the dynamic charge at a specific atom. We demonstrate the power of TR-XPS by using sulphur 2p-core-electron-emission probing to study the UV-excited dynamics of 2-thiouracil. The method allows us to discover that a major part of the population relaxes to the molecular ground state within 220–250 fs. In addition, a 250-fs oscillation, visible in the kinetic energy of the TR-XPS, reveals a coherent exchange of population among electronic states.


2018 ◽  
Vol 20 (7) ◽  
pp. 4901-4910 ◽  
Author(s):  
V. V. Mulloyarova ◽  
I. S. Giba ◽  
M. A. Kostin ◽  
G. S. Denisov ◽  
I. G. Shenderovich ◽  
...  

By using NMR in liquefied gases, the stoichiometry of hydrogen-bonded complexes is determined via H/D isotope effects on proton chemical shifts.


2018 ◽  
Vol 74 (5) ◽  
pp. 608-617 ◽  
Author(s):  
Mahsa Eghbali Toularoud ◽  
Mehrdad Pourayoubi ◽  
Michal Dušek ◽  
Václav Eigner ◽  
Krishnan Damodaran

The two single-enantiomer phosphoric triamides N-(2,6-difluorobenzoyl)-N′,N′′-bis[(S)-(−)-α-methylbenzyl]phosphoric triamide, [2,6-F2-C6H3C(O)NH][(S)-(−)-(C6H5)CH(CH3)NH]2P(O), denoted L-1, and N-(2,6-difluorobenzoyl)-N′,N′′-bis[(R)-(+)-α-methylbenzyl]phosphoric triamide, [2,6-F2-C6H3C(O)NH][(R)-(+)-(C6H5)CH(CH3)NH]2P(O), denoted D-1, both C23H24F2N3O2P, have been investigated. In their structures, chiral one-dimensional hydrogen-bonded architectures are formed along [100], mediated by relatively strong N—H...O(P) and N—H...O(C) hydrogen bonds. Both assemblies include the noncentrosymmetric graph-set motifs R 2 2(10), R 2 1(6) and C 2 2(8), and the compounds crystallize in the chiral space group P1. Due to the data collection of L-1 at 120 K and of D-1 at 95 K, the unit-cell dimensions and volume show a slight difference; the contraction in the volume of D-1 with respect to that in L-1 is about 0.3%. The asymmetric units of both structures consist of two independent phosphoric triamide molecules, with the main difference being seen in one of the torsion angles in the OPNHCH(CH3)(C6H5) part. The Hirshfeld surface maps of these levo and dextro isomers are very similar; however, they are near mirror images of each other. For both structures, the full fingerprint plot of each symmetry-independent molecule shows an almost asymmetric shape as a result of its different environment in the crystal packing. It is notable that NMR spectroscopy could distinguish between compounds L-1 and D-1 that have different relative stereocentres; however, the differences in chemical shifts between them were found to be about 0.02 to 0.001 ppm under calibrated temperature conditions. In each molecule, the two chiral parts are also different in NMR media, in which chemical shifts and P–H and P–C couplings have been studied.


1995 ◽  
Vol 103 (13) ◽  
pp. 5848-5859 ◽  
Author(s):  
Faris Gel’mukhanov ◽  
Hans Ågren

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