Paramagnetic nanoparticle T(1) and T(2) MRI contrast agents

There is no doubt that magnetic resonance imaging contrast agents (MRI CAs) can play a vital role in diagnosing diseases. Therefore, demand for new MRI CAs with an enhanced sensitivity and advanced functionalities is very high. Here, paramagnetic nanoparticles (NPs) are reviewed as new potential candidates for either T(1) or T(2) MRI CAs or both. These include surface coated lanthanide (Ln) oxide NPs (Ln = Gd, Dy, and Ho) and manganese oxide NPs. Surface coating materials should be biocompatible and hydrophilic. Compared to conventional large NPs, these surface coated paramagnetic NPs can be made ultrasmall with core particle diameter ranging from 1 to 3 nm, but their magnetic properties are still sufficient for MRI CAs. At this particle diameter, they can be easily excreted from the body through the renal system, which is prerequisite for in vivo applications. Mixed lanthanide oxide NPs into which a fluorescent Ln material is incorporated will be valuable as multiple imaging agents for both MRI-fluorescent imaging (FI) and MRI-cellular imaging (CL). These paramagnetic NPs can be further functionalized towards target-specific imaging, multiplex imaging, and drug delivery.     

Amide (A)–thioamide (T) interconversions using Ph3SiSH (A to T) and Ph3SnOH (T to A) reagents

Ph₃SiSH transforms amides to thioamides and Ph₃SnOH performs the reverse process, with the concomitant formation of Ph₃SiOH (or Ph₃SiOSiPh₃) and Ph₃SnSSnPh₃, respectively. The chemistry is a delightful illustration of the oxophilicity of silicon compared to the thiophilicity of tin and occurs under relatively mild conditions, and for amide to thioamide transformation requires no amide activation. The chemistry is in accord with available data for Si? (S)(O), Sn? (O)(S) and C?(O)(S) bond energies. Copyright © 2016 John Wiley & Sons, Ltd.     

Ein Titrationsverfahren von Quecksilber(II) mit Tetraphenyloborat (T)

Ohne Zusammenfassung     

Hydrogels Incorporating GdDOTA: Towards Highly Efficient Dual T(1) /T(2) MRI Contrast Agents

Do not tumble dry: Gadolinium-DOTA encapsulated into polysaccharide nanoparticles (GdDOTA?NPs) exhibited high relaxivity (r(1) =101.7?s(-1) mM(-1) per Gd(3+) ion at 37?°C and 20?MHz). This high relaxation rate is due to efficient Gd loading, reduced tumbling of the Gd complex, and the hydrogel nature of the nanoparticles. The efficacy of the nanoparticles as a T(1) /T(2) dual-mode contrast agent was studied in C6 cells.     

Structure of synthetic erionite (zeolite T)

Summary Zeolite T is a synthetic analog of the natural-occurring zeolite-erionite.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 6, pp. 1116–1118, June, 1965     

Extraktionsphotometrische Methode zur Rheniumbestimmung mit Hilfe von Safranin T (Saf T)

Analytical and Bioanalytical Chemistry -     

Superconductivity in LaT(M)BN and La3T(M2)B2N3 (T(M) = transition metal) synthesized under high pressure

Various layered boronitrides (LaN)(n)(T(M2)B(2)) (T(M) = transition metal; n = 2, 3) have been prepared using a high-pressure synthesis technique in which an inverse α-PbO-type T(M2)B(2) layer is separated by two or three rock salt-type LaN layers and these layers are connected through linear (BN) units. The electronic states of the distinguishing (BN) unit and intermediate rock salt-type LaN layer are discussed on the basis of density functional theory calculations. Bulk superconductivity has been found in LaNiBN (T(c) ≈ 4.1 K), CaNiBN (T(c) ≈ 2.2 K), and LaPtBN (T(c) ≈ 6.7 K), where the Fermi level E(F) is located in the bands composed of the T(M)(d)-B(2p) antibonding state and the main T(M)(d) band resides well below E(F). The non-superconductive T(M)-based compounds exhibit Pauli paramagnetic behavior, in which the highly itinerant nature of the electrons caused by strong T(M)(d)-B(2p) covalent bonding suppresses the long-range magnetic ordering.     

Unexpected A·T(WC)↔A·T(rWC)/A·T(rH) and A·T(H)↔A·T(rH)/A·T(rWC) conformational transitions between the classical A·T DNA base pairs: A QM/QTAIM comprehensive study

In this study, using QM/QTAIM calculations in the continuum with ε = 1 under normal conditions, we have revealed for the first time the nondissociative A·T(WC)↔A·T(rWC)/A·T(rH) and A·T(H)↔A·T(rH)/A·T(rWC) conformational transitions. It was established that they proceed via the essentially nonplanar transition states (С₁ symmetry) through the intermediates, which are wobbled conformers (С₁ symmetry) theoretically predicted in our previous work (Brovarets’ et al., Frontiers in Chemistry, 2018, 6:8, 10.3389/fchem.2018.00008) of the classical А·Т DNA base pairs—Watson–Crick А·Т(WC), reverse Watson–Crick А·Т(rWC), Hoogsteen А·Т(Н) and reverse Hoogsteen А·Т(rН). At this, the A·T(H)↔A·T(rWC) and A·T(WC)↔A·T(rH) conformational transformations are controlled by the transition states (TSs) stabilized by the participation of the intermolecular (T)N3H···N6(A) H‐bond (∼3.70 kcal·mol⁻¹) between the imino group N3H of T and pyramidilized amino group N6H₂ of A. Gibbs free energies of activation for these processes consist 12.22 and 11.11 kcal·mol⁻¹, accordingly, under normal conditions. TSs, which control the A·T(WC)↔A·T(rWC) and A·T(H)↔A·T(rH) conformational transitions are stabilized by the participation of the intermolecular (T)N3H···N6(A) H‐bond (5.82 kcal·mol⁻¹) and bifurcating intermolecular (T)N3H···N6(A) (5.00) and (T)N3H···N7(A) (0.61 kcal·mol⁻¹) H‐bonds, accordingly. Notably, in these two TSs amino group N6H₂ of A is significantly pyramidilized; Gibbs free energies of activation for these reactions are 19.07 and 19.71 kcal·mol⁻¹, accordingly.     

Magnetische Messungen in den Mischphasen (T I,T II)3 {Si,Ge}; (T I,T II=Fe,Co, Ni)

Solid solutions of silicides and germanides having BiF₃ and Cu₃Au type structure have been measured in the ferromagnetic and paramagnetic region in the range between 80 K and 1270 K. The results are discussed by means of a model given byLecocq et al. for Fe₃Si, in the case of the silicides and with a modified model in the case of the germanides.     

Improving upon CCSD(T): LambdaCCSD(T). II. Stationary formulation and derivatives

Analytical derivatives are formulated and implemented for the LambdaCCSD(T) method. As the historically first size-extensive and orbitally invariant extension of coupled-cluster (CC) theory to exploit the left-hand ground state eigenvector, it offers a vastly better treatment of bond breaking than does CCSD(T), and points the way toward further generalizations of single-reference CC theory that enhance its accuracy away from equilibrium geometries. Application to diatomic force curves and transition states of several well-characterized reactions are made. Surprisingly, despite LambdaCCSD(T) describing bond breaking much better than CCSD(T), for transition states both methods are extremely close in both structures and activation barriers. Force curves, however, demonstrate the overall superiority of LambdaCCSD(T).     

Liquid-state transitions (T>T g) of poly(vinyl alcohol)

The two liquid state transitions,T _ll andT _ll, of non-crystalline, uncrosslinked poly(vinyl alcohol) were determined by differential scanning calorimetry.T _ll increased as the molecular weightM _n increased, whileT _ll remained almost constant. Crosslinking and crystallinity lead to disappearance of the transitionT _ll. The transitionT _ll was linked to mobility of whole chains, whereasT _ll was characteristic of segmental mobility.     

Hole polarons in poly(G)-poly(C) and poly(A)-poly(T) DNA molecules

The polaron might play an important role in the process of charge migration through duplex DNA stack. In the present work, we investigate properties of hole polarons in DNA molecules containing identical base pairs, such as poly(G)-poly(C) and poly(A)-poly(T), An extended tight-binding model (extended Su-Schrieffer-Heeger model), which involves the effect of an electric field in the direction of DNA stack, will be introduced. The transfer integral and electron-phonon coupling parameters in this model are obtained according to ab initio calculation for different base pair dimers. Calculations reveal that the polaron in poly(A)-poly(T) has a wider shape and a higher mobility under a specific electric field than that in poly(G)-poly(C) DNA stack.     

Substitution and hydrogenation reactions on rhodium(I)-ethylene complexes of the hydrotris(pyrazolyl)borate ligands T (T = Tp, TpMe2)

The bis(ethylene) Rh species TpMe2Rh(C2H4)2(1*) (TpMe2 = tris(3,5-dimethyl-1-pyrazol-1-yl)hydroborate) has been obtained from [RhCl(C2H4)2]2 and KTpMe2. Complex 1* easily decomposes in solution to give mainly the butadiene species TpMe2Rh(eta74-C4H6). In the solid state its thermal decomposition follows a different course and the allyl TpMe2RhH(syn-C3H4Me) is cleanly obtained as a mixture of exo and endo isomers. The complexes Tp'Rh(C2H4)2 (Tp' = Tp, TpMe2) afford the monosubstituted species Tp'Rh(C2H4)(PR3) upon reaction with PR3 but react differently with L = CO or CNR: the Tp compound gives dinuclear [TpRh]2(mu-L)3 complexes, while, in the case of 1*, TpMe2Rh(C2H4)(L) species are obtained. The ethylene ligand of complexes TpMe2Rh(C2H4)(PR3) is labile, and several peroxo compounds of composition TpMe2Rh(O2)(PR3) have been isolated by their reaction with O2. All the mononuclear Rh(I) complexes are formulated as 18e- trigonal bipyramidal species on the basis of IR and NMR spectroscopic studies. A series of dihydride complexes of Rh(III) of formulation Tp'RhH2(PR3) have been prepared by the hydrogenation of the corresponding ethylene derivatives. Complexes [TpRh]2(mu-CNCy)3, TpMe2Rh(C2H4)(PEt3), and TpMe2Rh(O2)(PEt3) have been further characterized by X-ray diffraction studies.