Tatiana Timofeeva

Dr. Tatiana Timofeeva


Research Focus & Metrics

Academic Career Length

31Years (1996-Present)

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

Representative Publications

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11 April 2013 in CrystEngComm
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SDSergiu Draguta
Sergiu Draguta
MFMarina S. Fonari
Marina S. Fonari
AMArtem Masunov
Artem Masunov
JZJoel Zazueta
Joel Zazueta
SSShannon Sullivan
Shannon Sullivan
TTTatiana Timofeeva
Tatiana Timofeeva
Co-crystallization of 4-nitrophenol (I) with five aminopyridines (4-aminopyridine 1, 3,4-diaminopyridine 2, 2,3-diaminopyridine 3, 3-aminopyridine 4, 2-amino-6-methylpyridine 5) and 2,4-diaminopyrimidine 6 resulted in six adducts with the ratio of components 2 : 1 in five and 1 : 1 in one final compounds. Single crystals were grown by slow evaporation technique using ethanol as a solvent. Five adducts with 1–5 crystallize in acentric P21 and Pna21 space groups, and one, 2(I)·6 – in centrosymmetric P21/c space group. Compounds 2(I)·1, 2(I)·2, 2(I)·3 are isomorphous, and demonstrate similar H-bonding patterns despite the differences in aminopyridine molecules. Compound 2(I)·5 is isomorphous to two previously reported compounds. Adducts 2(I)·1, 2(I)·2, 2(I)·3, 2(I)·5, 2(I)·6 represent organic salts composed of pyridinium/pyrimidinium cation, 4-nitrophenolate anion, and 4-nitrophenol neutral molecule. The H-bonded 4-nitrophenol–4-nitrophenolate anionic dimers were found in all compounds with 2 : 1 molar ratio. In adduct I·4 both molecules are in neutral form. The IR spectral data support crystallographic conclusions on salts formation. Plane wave pseudopotential density functional theory calculations were used to predict hyperpolarizability tensor components. Our calculations suggest 2(I)·3 as the best candidate for nonlinear optical materials (14 times more active than urea).

9 October 2019 in Advanced Functional Materials
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RDRaghunath R. Dasari
Raghunath R. Dasari
XWXu Wang
Xu Wang
RWRen A. Wiscons
Ren A. Wiscons
HHHamna F. Haneef
Hamna F. Haneef
AAAjith Ashokan
Ajith Ashokan
SMSeth Marder
Seth Marder

19 January 2022 in Chemistry of Materials
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Journal Article
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MTMarie-Hélène Tremblay
Marie-Hélène Tremblay
ABAllyson Boyington
Allyson Boyington
SRSergei Rigin
Sergei Rigin
JJJie Jiang
Jie Jiang
JBJohn Bacsa
John Bacsa
SMSeth Marder
Seth Marder

31 March 2010 in European Journal of Medicinal Chemistry
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Journal Article
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MMMikhail Makarov
Mikhail Makarov
ELEvgeniya S. Leonova
Evgeniya S. Leonova
EREkaterina Yu. Rybalkina
Ekaterina Yu. Rybalkina
PTPaul Tongwa
Paul Tongwa
VKVictor N. Khrustalev
Victor N. Khrustalev
IOIrina L. Odinets
Irina L. Odinets

6 December 2013 in Dalton Transactions
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CBChristina Bauer
Christina Bauer
SJSimon C. Jones
Simon C. Jones
TKTiffany L. Kinnibrugh
Tiffany L. Kinnibrugh
PTPaul Tongwa
Paul Tongwa
RFRichard A. Farrell
Richard A. Farrell
MAMark D. Allendorf
Mark D. Allendorf
Metal–organic frameworks (MOFs) can provide a matrix for the assembly of organic chromophores into well-defined geometries, allowing for tuning of the material properties and study of structure–property relationships. Here, we report on the effect of the coordinated metal ion on the luminescence properties of eight isostructural MOFs having the formula M1 2M2L3(DMF)2 (M1 = M2 = Zn (1), Cd (2), Mn (3), Co (4); M1 = Zn, M2 = Cd (5), Mn (6), Co (7); M1 = Co, M2 = Mn (8); L = trans-4,4′-stilbene dicarboxylate), synthesized by reaction of the appropriate metal nitrate or mixtures of metal nitrates with LH2 in DMF. The crystal structures of 2, 3 and 5–8 were determined by X-ray diffraction to be composed of trinuclear metal clusters linked by stilbene dicarboxylate linkers in a paddlewheel geometry, extending to form a 2-D layered structure. In the mixed-metal cases, the larger metal ion was found to occupy the octahedral site in the cluster while the smaller ion occupies the tetrahedral positions, suggesting a selective, ligand-directed assembly process for the mixed-metal species. Variable temperature magnetic measurements for paramagnetic MOFs 3 and 6–8 were consistent with the site occupancies determined crystallographically, and indicated weak intra-cluster antiferromagnetic coupling for 3 and 8. Comparison between the crystal structures of 2, 3 and 5–8 and those reported for 1 and 4 in the literature reveal close resemblances between linker environments, with important intermolecular stilbene–stilbene geometries that are comparable in all cases. Interestingly, pale-colored 1–3 and 5–7 display very similar emission profiles upon excitation at λex = 350 nm, whereas dark-colored 4 and 8 do not exhibit detectable emission spectra. The bright, well-resolved luminescence of 1, 2 and 5 is ascribed to rigidification of the linker upon coordination to the d10 metal ions, whereas the weaker emission observed for 3, 6 and 7 is presumably a result of quenching due to close proximity of the linker to one or more paramagnetic ions. Time-resolved measurements for 1, 2, 5 and 6 reveal biexponential emission decays, where the lifetime of the longer-lived state corresponds to observed variations in the nearest-neighbor cofacial stilbene–stilbene distances in their crystal structures. For 3, a monoexponential decay with shorter lifetime was determined, indicating significant paramagnetic quenching of its emissive state.

26 September 2014 in Crystal Growth & Design
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COCarlos Ordonez
Carlos Ordonez
MFMarina Fonari
Marina Fonari
JLJennifer Lindline
Jennifer Lindline
QWQiang Wei
Qiang Wei
TTTatiana Timofeeva
Tatiana Timofeeva