0000000001303196
AUTHOR
Daniel Fortin
showing 61 related works from this author
Reactivity of CuI and CuBr toward Et2S: a reinvestigation on the self-assembly of luminescent copper(I) coordination polymers.
2010
CuI reacts with SEt(2) in hexane to afford the known strongly luminescent 1D coordination polymer [(Et(2)S)(3){Cu(4)(mu(3)-I)(4)}](n) (1). Its X-ray structure has been redetermined at 115, 235, and 275 K in order to address the behavior of the cluster-centered emission and is built upon Cu(4)(mu(3)-I)(4) cubane-like clusters as secondary building units (SBUs), which are interconnected via bridging SEt(2) ligands. However, we could not reproduce the preparation of a coordination polymer with composition [(Et(2)S)(3){Cu(4)(mu(3)-Br)(4)}](n) as reported in Inorg. Chem. 1975, 14, 1667. In contrast, the autoassembly reaction of SEt(2) with CuBr results in the formation of a novel 1D coordination…
The first unpaired electron placed inside a C3-symmetry P-chirogenic cluster
2010
The Pd(3)(dppm*)(3)(CO)(n+) enantiomers (n = 2 (2), 1 (3)) were prepared either from (R,R)- or (S,S)-P-chirogenic bis(phenyl-m-xylylphosphino)methane (dppm*; 1) and Pd(OAc)(2) in the presence of CF(3)CO(2)H, CO and water (n = 2), and then by reductive electrolysis (n = 1). The stable enantiomeric [Pd(3)((S,S)-dppm*)(3)(CO)](+)˙ (3), is the first C(3)-symmetry radical-cation M-M bonded cluster, therefore the odd electron is delocalized onto the Pd(3) frame within this symmetry. The novel chiral species have been characterized by circular dichroism (CD) of both enantiomers of the Pd(3)(dppm*)(3)(CO)(2+) clusters (2) and by EPR spectroscopy for the Pd(3)((S,S)-dppm*)(3)(CO)(+)˙ paramagnetic co…
Decoupling the artificial special pair to slow down the rate of singlet energy transfer
2012
Trimer 2, composed of a cofacial heterobismacrocycle, octamethyl-porphyrin zinc(II) and bisarylporphyrin zinc(II) held by an anthracenyl spacer, and a flanking acceptor, bisarylporphyrin free-base ( Ar = -3,5-(t Bu )2 C 6 H 3), has been studied by means of absorption spectroscopy, "steady state and time-resolved fluorescence" and fs transient absorption spectroscopy, and density functional theory (DFT) in order to assess the effect of decoupling the chromophores' low energy MOs on the rate of the singlet, S1, energy transfer, k ET , compared to a recently reported work on a heavily coupled trimeric system, Trimer 1, [biphenylenebis(n-nonyl)porphyrin zinc(II)]-bisarylporphyrin free-base ( A…
Copper(I) Halides (X = Br, I) Coordinated to Bis(arylthio)methane Ligands: Aryl Substitution and Halide Effects on the Dimensionality, Cluster Size a…
2014
Bis(phenylthio)methane (L1) reacts with CuI to yield the 1D-coordination polymer [{Cu4(μ3-I)4}(μ-L1)2]n (1) bearing cubane Cu4I4 clusters as connecting nodes. The crystal structures at 115, 155, 195, and 235 K provided evidence for a phase transition changing from the monoclinic space group C2/c to P21/c. The self-assembly process of CuI with bis(p-tolylthio)methane (L2), bis(4-methoxyphenylthio)methane (L3), and bis(4-bromo-phenylthio)methane (L4) affords the 1D-coordination polymers [{Cu4(μ3-I)4}(μ-Lx)2]n (x = 2, 3, or 4). Compounds 2 and 4 are isostructural with C2/c low temperature polymorph of 1, whereas the inversion centers and 2-fold axes are lost in 3 (space group Cc). The use of b…
Luminescent P-Chirogenic Copper Clusters
2013
P-chirogenic clusters of the cubanes [Cu4I4L4] (L = chiral phosphine) were prepared from (+)- and (-)-ephedrine with L = (S)- or (R)-(R)(Ph)(i-Pr)P (with R = CH3 (seven steps) or C17H35 (10 steps)) with e.e. up to 96%. The X-ray structure of [Cu4I4((R)-(CH3)(Ph)(i-Pr)P)4] confirmed the cubane structure with average Cu···Cu and Cu···I distances of 2.954 and 2.696 Å, respectively. The cubane structure of the corresponding [Cu4I4((S)-(CH3)(Ph)(i-Pr)P)4] was established by the comparison of the X-ray powder diffraction patterns, and the opposite optical activity of the (S)- and (R)-ligand-containing clusters was confirmed by circular dichroism spectroscopy. Small-angle X-ray scattering patterns…
The Pd3(dppm)3(CO)n clusters (n = 1-,2-); rare cases of anionic palladium species.
2010
Two novel anionic palladium clusters, Pd(3)(dppm)(3)(CO)(n-) (Pd(3)(n); n = 1-,2-) were electrochemically generated from the dicationic cluster Pd(3)(2+) in 0.2 M THF/Bu(4)NPF(6)via two first consecutive reversible 1-electron reductions (Pd(3)(2+) + 1 e(-) ⇌ Pd(3)(+), -0.210, and Pd(3)(+) + 1 e(-) ⇌ Pd(3)(0), -0.470 V vs. SCE) followed by two others at -2.350 (Pd(3)(0) + 1 e(-) ⇌ Pd(3)(1-), reversible) and at -2.690 V vs. SCE (Pd(3)(1-) + 1 e(-) ⇌ Pd(3)(2-), irreversible). The chemical stability and instability, respectively, of the Pd(3)(dppm)(3)(CO)(n-) clusters (Pd(3)(n); n = 1-,2-) at the time scale of the electrochemical experiments were addressed by DFT computations. Indeed, geometry …
P-Chirogenic Phosphines Supported by Calix[4]arene: New Insight into Palladium-Catalyzed Asymmetric Allylic Substitution
2013
The first P-chirogenic mono- and diphosphine ligands supported on the upper rim of a calix[4]arene moiety were synthesized using the ephedrine methodology. The lithiated calix[4]arene mono- and dianions both react with the oxazaphospholidine–borane, prepared from ephedrine, to afford regio- and stereoselectively the corresponding calix[4]arenyl aminophosphine–boranes, by cleavage of the heterocyclic ring at the P–O bond position. Subsequent reactions with HCl and then organolithium reagent and finally decomplexation with DABCO lead to the corresponding calix[4]arenyl mono- or diphosphines. Both enantiomers of the calix[4]arenyl phosphines were obtained either by using (+)- or (−)-ephedrine …
Design of Triads for Probing the Direct Through Space Energy Transfers in Closely Spaced Assemblies
2013
Using a selective stepwise Suzuki cross-coupling reaction, two trimers built on three different chromophores were prepared. These trimers exhibit a D(^)A1-A2 structure where the donor D (octa-β-alkyl zinc(II)porphyrin either as diethylhexamethyl, 10a, or tetraethyltetramethyl, 10b, derivatives) through space transfers the S1 energy to two different acceptors, di(4-ethylbenzene) zinc(II)porphyrin (A1; acceptor 1) placed cofacial with D, and the corresponding free base (A2; acceptor 2), which is meso-meso-linked with A1. This structure design allows for the possibility of comparing two series of assemblies, 9a,b (D(^)A1) with 10a,b (D(^)Â1-A2), for the evaluation of the S1 energy transfer for…
Through-bond versus through-space T1 energy transfers in organometallic compound-metalloporphyrin pigments
2009
The preparation and characterization of two d9−d9 M2-bonded Pt2(dppm)2(C≡CC6H4-M(P))2 complexes (where M = Zn or Pd, and P = diethylhexamethylporphyrin) were achieved. The central [Pt2(dppm)2(C≡CC6H4)2] organometallic unit appears to be an independent chromophore and is suspected to be luminescent at 77 K (in 2MeTHF) in the porphyrin-containing complexes, as this is the case for the unfunctionalized Pt2(dppm)2(C≡CPh)2 parent compound. However, when this spacer is connected (by a single C−C bond) to either M(P) (M = Zn, Pd), even in the absence of conjugation (as the computed dihedral angle between the C6H4 and porphyrin planes is ∼84.5°), total quenching of the luminescence of the [Pt2(dppm…
The First P ‐Stereogenic 1D Coordination Polymers with the Metal Centers in the Backbone
2011
The enantiomeric ligands (R,R)- and (S,S)-bis(o-anisylphenylphosphanyl)methane (R,R-22 and S,S-22) and (R,R)- and (S,S)-bis(phenyl-m-xylylphosphanyl)methane (R,R-23 and S,S-23; dppm*), were treated with [Cu(NCCH3)4](BF4) and AgBF4 to produce the binuclear complexes [Cu2(dppm*)2(NCCH3)4](BF4)2 or [Ag2(dppm*)2](BF4)2, respectively. Then, these complexes were used as building blocks to prepare the first P-chirogenic 1D coordination polymers {[M2(dppm*)2(dmb)2](BF4)2}n [dppm* = (R,R)-22, (S,S)-22, (R,R)-23, (S,S)-23, M = Cu, Ag, dmb = 1,8-diisocyano-p-menthane] where M is part of the backbone of the polymer chain. The isostructural nature of these new polymers with the achiral parent polymers, …
A Very Low Band Gap Diketopyrrolopyrrole-Porphyrin Conjugated Polymer
2017
International audience; A porphyrin-diketopyrrolopyrrole-containing polymer (poly(porphyrin-diketopyrrolopyrrole) (PPDPP)) shows impressive molar absorption coefficients from lambda=300 to 1000 nm. The photophysical and structural properties of PPDPP have been studied. With PPDPP as the electron donor and [ 6,6]phenyl C-71 butyric acid methyl ester (PC71BM) as the electron acceptor, the bulk heterojunction polymer solar cell showed overall power conversion efficiencies of 4.18 and 6.44% for as-cast and two-step annealing processed PPDPP: PC71BM (1: 2) active layers, respectively. These results are quite impressive for porphyrin-containing polymers, especially when directly included in the p…
Formation of an unprecedented (CuBr)5 cluster and a zeolite-type 2D-coordination polymer: a surprising halide effect
2013
A unique pentanuclear cluster within a zeolite-type polymer ([Cu5(μ4-Br)(μ3-Br)2(μ2-Br)2](μ2-MeSPr)3)n (1; void space >81%) and a luminescent 1D ([Cu(μ3-I)]4(MeSPr)3)n polymer, 2, are formed when MeSPr reacts with CuBr and CuI.
1,4-Bis(arylthio)but-2-enes as Assembling Ligands for (Cu2X2)n (X = I, Br; n = 1, 2) Coordination Polymers: Aryl Substitution, Olefin Configuration, …
2016
CuI reacts with E-PhS(CH2CH═CHCH2)SPh, L1, to afford the coordination polymer (CP) [Cu2I2{μ-E-PhS(CH2CH═CHCH2)SPh}2]n (1a). The unprecedented square-grid network of 1 is built upon alternating two-dimensional (2D) layers with an ABAB sequence and contains rhomboid Cu2(μ2-I)2 clusters as secondary building units (SBUs). Notably, layer A, interconnected by bridging L1 ligands, contains exclusively dinuclear units with short Cu···Cu separations [2.6485(7) A; 115 K]. In contrast, layer B exhibits Cu···Cu distances of 2.8133(8) A. The same network is observed when CuBr reacts with L1. In the 2D network of [Cu2Br2{μ-E-PhS(CH2CH═CHCH2)SPh}2]n (1b), isotype to 1a, one square-grid-type layer contain…
Strong donor–acceptor couplings in a special pair-antenna model
2010
A special pair model composed of two cofacial zinc porphyrins (acceptor) linked to a free base (donor) acts as an energy transfer dyad. Despite the absence of conjugation, ππ*/charge transfer excited states and ultrafast energy transfer (∼5 ps) are noted.
Organometallic Oligomers Based on Bis(arylacetylide)bis(P-chirogenic phosphine)platinum(II) Complexes: Synthesis and Photonic Properties
2013
A series of P-chirogenic oligomers of the type (-C≡C-aryl-C≡C-PtL2-)n [L = (R)- and (S)-P(Ph)(iPr)(C17H35); aryl = 1,4-benzene, 2,1,3-benzothiadiazole] along the corresponding achiral analogues (L = PBu3) and model complexes PhC≡CPtL2C≡CPh were prepared from the ephedrine strategy and were fully characterized [(1)H, (31)P NMR; IR; small-angle X-ray scattering (SAXS); gel permeation chromatography (GPC); thermal gravimetric analysis (TGA); circular dichroism, UV-vis, and luminescence spectroscopy; photophysics, and degree of anisotropy measurements]. From the CD measurements, the chiral environment of the phosphine ligands is modestly felt by the aryl moieties. Concurrently, the TGA shows th…
Singlet and triplet energy transfers in tetra-(meso-truxene)zinc(II)- and tetra-(meso-tritruxene)zinc(II) porphyrin and porphyrin-free base dendrimer…
2011
The synthesis, optical properties, and energy transfer features of four dendrimers composed of meso-tetrasubstituted zinc(II) porphyrin (ZnP) or a free base (P) central core, where the substituents are four truxene (Tru) or four tritruxene dendrons (TriTru), TruP, TriTruP, TruZnP, and TriTruZnP, are reported. Selective excitation of the truxene donors results in a photoinduced singlet energy transfer from the truxenes to the porphyrin acceptor. The rates for singlet energy transfer (k(ET)), evaluated from the change in the fluorescence lifetime of the donors (Tru and TriTru) in the presence and absence of the acceptor (P or ZnP) for TruP, TruZnP, TriTruP, and TriTruZnP, are 5.9, 1.2, 0.87, …
CCDC 1418779: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 952665: Experimental Crystal Structure Determination
2013
Related Article: Naima Khiri-Meribout, Etienne Bertrand, Jérôme Bayardon, Marie-Joëlle Eymin, Yoann Rousselin, Hélène Cattey, Daniel Fortin, Pierre D. Harvey, and Sylvain Jugé|2013|Organometallics|32|2827|doi:10.1021/om400229p
CCDC 974338: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 974340: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 1418785: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418780: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 974327: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 1418767: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418763: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418781: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418772: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 974334: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 1418782: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418770: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418765: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 974333: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 947670: Experimental Crystal Structure Determination
2013
Related Article: Antony Lapprand, Antoine Bonnot, Michael Knorr, Youann Rousselin, Marek M. Kubicki, Daniel Fortin, Pierre D. Harvey|2013|Chem.Commun.|49|8848|doi:10.1039/C3CC45284K
CCDC 1418776: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1424523: Experimental Crystal Structure Determination
2015
Related Article: Antony Lapprand, Mathieu Dutartre, Naïma Khiri, Etienne Levert, Daniel Fortin, Yoann Rousselin, Armand Soldera, Sylvain Jugé and Pierre D. Harvey|2013|Inorg.Chem.|52|7958|doi:10.1021/ic400498j
CCDC 1418784: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 974326: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 974341: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 974324: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 1418769: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 974325: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 1418774: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418783: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418771: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 974328: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 1418766: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 974336: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 974335: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 1418764: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418775: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 974337: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 1418762: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 952664: Experimental Crystal Structure Determination
2013
Related Article: Naima Khiri-Meribout, Etienne Bertrand, Jérôme Bayardon, Marie-Joëlle Eymin, Yoann Rousselin, Hélène Cattey, Daniel Fortin, Pierre D. Harvey, and Sylvain Jugé|2013|Organometallics|32|2827|doi:10.1021/om400229p
CCDC 974329: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 1431598: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418773: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 1418768: Experimental Crystal Structure Determination
2016
Related Article: Antoine Bonnot, Michael Knorr, Fabrice Guyon, Marek M. Kubicki, Yoann Rousselin, Carsten Strohmann, Daniel Fortin, Pierre D. Harvey|2016|Cryst.Growth Des.|16|774|doi:10.1021/acs.cgd.5b01360
CCDC 952663: Experimental Crystal Structure Determination
2013
Related Article: Naima Khiri-Meribout, Etienne Bertrand, Jérôme Bayardon, Marie-Joëlle Eymin, Yoann Rousselin, Hélène Cattey, Daniel Fortin, Pierre D. Harvey, and Sylvain Jugé|2013|Organometallics|32|2827|doi:10.1021/om400229p
CCDC 974339: Experimental Crystal Structure Determination
2014
Related Article: Michael Knorr,Abderrahim Khatyr,Ahmed Dini Aleo,Anass El Yaagoubi,Carsten Strohmann,Marek M. Kubicki,Yoann Rousselin,Shawkat M. Aly,Antony Lapprand,Daniel Fortin, Pierre D. Harvey|2014|Cryst.Growth Des.|14|5373|doi:10.1021/cg500905z
CCDC 952662: Experimental Crystal Structure Determination
2013
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