Svetlana Baca

Dr. Svetlana Baca

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Research Focus & Metrics

Academic Career Length

26Years (2001-Present)

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

Representative Publications

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1 March 2006 in Polyhedron
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Journal Article
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SBSvetlana Baca
Svetlana Baca
MRManfred T. Reetz
Manfred T. Reetz
RGRichard Goddard
Richard Goddard
IFIrina G. Filippova
Irina G. Filippova
YSYurii A. Simonov
Yurii A. Simonov
NGNicolae Gerbeleu
Nicolae Gerbeleu

30 September 2011 in Chemical Communications
Verified
Journal Article
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IMIurii L. Malaestean
Iurii L. Malaestean
AEArkady Ellern
Arkady Ellern
SBSvetlana Baca
Svetlana Baca
PKPaul Kögerler
Paul Kögerler
High-nuclearity cerium oxide clusters do exist: condensation reactions starting from cerium coordination polymers result in ligand-terminated {Ce III/IV 10 } and {Ce III/IV 22 } oxide clusters, which exhibit formation and structural aspects that are partly similar and partly contrary to classical polyoxometalate chemistry.

1 September 2004 in Inorganica Chimica Acta
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Journal Article
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SBSvetlana Baca
Svetlana Baca
IFIrina G. Filippova
Irina G. Filippova
OGOlesea A. Gherco
Olesea A. Gherco
MGMaria Gdaniec
Maria Gdaniec
YSYurii A. Simonov
Yurii A. Simonov
SDSilvio Decurtins
Silvio Decurtins

28 October 2008 in Inorganic Chemistry
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Journal Article
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SBSvetlana Baca
Svetlana Baca
IMIurii L. Malaestean
Iurii L. Malaestean
TKTony Keene
Tony Keene
HAHarry Adams
Harry Adams
Michael WardMichael Ward
Michael Ward
SDSilvio Decurtins
Silvio Decurtins

30 January 2017 in Inorganic Chemistry
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Journal Article
Open access
OBOlga Botezat
Olga Botezat
JLJan van Leusen
Jan van Leusen
VKVictor Kravtsov
Victor Kravtsov
PKPaul Kögerler
Paul Kögerler
SBSvetlana Baca
Svetlana Baca
A family of wheel-shaped charge-neutral heterometallic {FeIII4LnIII2}- and {FeIII18MIII6}-type coordination clusters demonstrates the intricate interplay of solvent effects and structure-directing roles of semiflexible bridging ligands. The {Fe4Ln2}-type compounds [Fe4Ln2(O2CCMe3)6(N3)4(Htea)4]·2(EtOH), Ln = Dy (1a), Er (1b), Ho (1c); [Fe4Tb2(O2CCMe3)6(N3)4(Htea)4] (1d); [Fe4Ln2(O2CCMe3)6(N3)4(Htea)4]·2(CH2Cl2), Ln = Dy (2a), Er (2b); [Fe4Ln2(O2CCMe3)4(N3)6(Htea)4]·2(EtOH)·2(CH2Cl2), Ln = Dy (3a), Er (3b) and the {Fe18M6}-type compounds [Fe18M6(O2CCHMe2)12(Htea)18(tea)6(N3)6]·n(solvent), M = Dy (4, 4a), Gd (5), Tb (6), Ho (7), Sm (8), Eu (9), and Y (10) form in ca. 20–40% yields in direct reaction of trinuclear FeIII pivalate or isobutyrate clusters, lanthanide/yttrium nitrates, and bridging triethanolamine (H3tea) and azide ligands in different solvents: EtOH for the smaller {Fe4Ln2} wheels and MeOH/MeCN or MeOH/EtOH for the larger {Fe18M6} wheels. Single-crystal X-ray diffraction analyses revealed that 1–3 consist of planar centrosymmetric hexanuclear clusters built from FeIII and LnIII ions linked by an array of bridging carboxylate, azide, and aminopolyalcoholato-based ligands into a cyclic structure with a cavity, and with distinct sets of crystal solvents (2 EtOH per formula unit in 1a–c, 2 CH2Cl2 in 2, and 2 EtOH and 2 CH2Cl2 in 3). In 4–10, the largest 3d/4f wheels currently known, nearly linear Fe3 fragments are joined via mononuclear Ln/Y units by a set of isobutyrates and amino alcohol ligands into virtually planar rings. The magnetic properties of 1–10 reveal slow magnetization relaxation for {Fe4Tb2} (1d) and slow relaxation for {Fe4Ho2} (1c), {Fe18Dy6} (4), and {Fe18Tb6} (6).

5 April 2007 in Dalton Transactions
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Journal Article
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SBSvetlana Baca
Svetlana Baca
HAHarry Adams
Harry Adams
DSDaniel Sykes
Daniel Sykes
SFStephen Faulkner
Stephen Faulkner
Michael WardMichael Ward
Michael Ward
A series of cyanide-bridged coordination networks has been prepared which contain [Ru(phen)(CN)4]2− anions, Ln(III) cations, and additional oligopyridine ligands (1,10-phenanthroline, 2,2′:6′,2‴-terpyridine or 2,2′-bipyrimidine) which coordinate to the Ln(III) centres. Five structural types have been identified and examples of each type of structure are described: these are hexanuclear Ru4Ln2 clusters; two-dimensional Ru–Ln sheets with a honeycomb pattern of edge-linked Ru6Ln6 hexagons; one-dimensional chains consisting of two parallel cross-linked strands in a ladder-like arrangement; simple single-stranded chains of alternating Ru/Ln components; and a one-dimensional ‘chain of squares’ in which Ru2Ln2 squares are linked by bipyrimidine bridging ligands which connect to the Ln(III) corners of adjacent squares in the sequence. The 3MLCT luminescence characteristic of the [Ru(phen)(CN)4]2− units is quenched in those networks containing Ln(III) which have low-lying near-infrared luminescent f–f states [Pr(III), Nd(III), Er(III), Yb(III)], with sensitised Ln(III)-based near-IR luminescence generated by d → f energy-transfer. The rate of d → f energy-transfer, and hence the degree of quenching of the 3MLCT luminescence from the [Ru(phen)(CN)4]2− units, depends on the availability of f–f levels of an appropriate energy on the Ln(III) centre, with Nd(III) (with a high density of low-lying f–f states) being the most effective energy-acceptor and Yb(III) (with a single low-lying f–f state) being the least effective. Rates of d → f energy-transfer to different Ln(III) centres could be determined from both the residual (partially quenched) lifetimes of the 3MLCT luminescence, and—in the case of the Yb(III) networks—by a rise-time for the sensitised near-IR luminescence. The presence of the ‘blocking’ polypyridyl ligands, which reduced the number of cyanide and water ligands that would otherwise coordinate to the Ln(III) centres, resulted in increases in the Ln(III)-based emission lifetimes compared to networks where these blocking ligands were not used.