Bedeutung der GC-Detektoreigenschaften

Ohne Zusammenfassung

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Enthalpies de formation de l'acide fluorhydrique dans les solutions ternaires HF/HX/H2O (HX = HCl, H2SO4) IV — Enthalpies de formation de l'acide fluorhydrique dans les solutions ternaires H2SO4/HF/H2O

The enthalpies of mixing of aqueous hydrofluoric and sulfuric acids and the enthalpies of dilution of the ternary solutions HF/H₂SO₄/H₂O at fixed concentration of HF or H₂SO₄ have been measured. The standard enthalpies of formation of HF in these solutions have been derived.     

CHEMILUMINESCENCE FROM AUTOXIDIZING 6-HYDROXYDOPAMINE: THE INVOLVEMENT OF ACTIVATED FORMS OF OXYGEN

Abstract— The autoxidation of the catecholamine neurotoxin 6-hydroxydopamine (20 μ M ) gave rise to a chemiluminescence which was greatly stimulated by FeSO₄ (20 μ M ) or by hydrogen peroxide addition (20 μ M to 2 m M ). The luminescence of both 6-hydroxydopamine alone or 6-hydroxydopamine plus hydrogen peroxide was strongly inhibited by catalase and by superoxide dismutase (both at 10 μg/m/); bovine serum albumin at 10 μg/m/ had no inhibitory effect. The luminescence was also strongly inhibited by several potent hydroxyl radical trapping agents and also by low concentrations of the ¹O₂ quencher DABCO (l,4-diazabicyclo-2.2.2.-octane). Chemiluminescence was greatly enhanced in D₂O, a solvent in which ¹O₂ has a prolonged lifetime. These data demonstrate the involvement of hydrogen peroxide, the superoxide radical and the hydroxyl radical in the chemiluminescence. The data are also consistent with some role for ¹O₂.     

Insertion reactions of GaCp*, InCp* and In[C(SiMe3)3] into the Ru-Cl bonds of [(p-cymene)RuIICl2]2 and [Cp*RuIICl]4

The first carbonyl free ruthenium/low valent Group 13 organyl complexes are presented, obtained by insertion of ER (ER = GaCp*, InCp*, In[C(SiMe(3))(3)]) into the Ru-Cl bonds of [(p-cymene)RuCl2]2, [Cp*RuCl]4 and [Cp*RuCl2]2. The compound [(p-cymene)RuCl2]2 reacts with GaCp*, giving a variety of isolated products depending on the reaction conditions. The Ru-Ru dimers [{(p-cymene)Ru}2(GaCp*)4(mu3-Cl)2] and the intermediate [{(p-cymene)Ru}2(mu-Cl)2] were isolated, as well as monomeric complexes [(p-cymene)Ru(GaCp*)3Cl2], [(p-cymene)Ru(GaCp*)2GaCl3] and [(p-cymene)Ru(GaCp*)2Cl2(DMSO)]. The reaction of [Cp*RuCl]4 with ER gives "piano-stool" complexes of the type [Cp*Ru(ER)3Cl](ER = InCp*, In[C(SiMe3)3], GaCp*. The chloride ligand in complex can be removed by NaBPh4, yielding [Cp*Ru(GaCp*)3]+[BPh4]-. The reaction of [Cp*RuCl2]2 with GaCp* however, does not lead to an insertion product, but to the ionic Ru(II) complex [Cp*Ru(GaCp*)3]+[Cp*GaCl3]-. The ER ligands in complexes 3, 5, 6, 7 and 8 are equivalent on the NMR timescale in solution due to a chloride exchange between the three Group 13 atoms even at low temperatures. The solid state structures, however, exhibit a different structural pattern. The chloride ligands exhibit two coordination modes: either terminal or bridging. The new compounds are fully characterized including single crystal X-ray diffraction. These results point out the different reactivities of the two precursors and the nature of the neutral p-cymene and the anionic Cp* ligand when bonding to a Ru(II) centre.     

An Anionic Amido-Substituted Seven-Vertex Siliconoid Cluster

The silanide [Si₄{N(SiMe₃)Dipp}₃]⁻ ( 1 ) transforms into the anionic siliconoid cluster [Si₇{N(SiMe₃)Dipp}₃]⁻ ( 2 ) with four unsubstituted silicon atoms as a contact ion pair with [K([18]crown-6)] in C₆D₆ at room temperature within five weeks. Anion 2 was investigated by natural population analysis and visualization of intrinsic atomic orbitals. Magnetically induced current-density calculations of 2 revealed two distinct strong diatropic vortices that sum up in one direction and create a strongly shielded apical silicon atom in 2 .     

Magnet design with high B(0) homogeneity for fast-field-cycling NMR applications

The design, construction, and performance of a low-inductance solenoidal coil with high B(0) homogeneity for fast-field-cycling NMR is presented. It consists of six concentric layers. The conductor width is varied to minimize the B(0) inhomogeneity in the volume of the sample. This is done using an algorithm which takes the real shape of the conductor directly into account. The calculated coil geometry can be manufactured easily using standard computerized numeric control equipment, which keeps the costs low. The coil is liquid cooled and produces a B(0) field of 0.95 T at 800 A. The field inhomogeneity in a cylindrical volume (diameter 5 mm, length 10 mm) is about 10 ppm, and the inductance is 190 microH. Switching times below 200 micros can be achieved. During 6 months of operation the coil has shown good stability and reliability.     

Recombination and transport in microcrystalline pin solar cells studied with pulsed electrically detected magnetic resonance

An analysis of spin-dependent processes in microcrystalline silicon (μc-Si:H) pin solar cells is presented using pulsed electrically detected magnetic resonance (pEDMR). In this first study it is shown that by modulating the morphology of the n-type contact layer from amorphous to microcrystalline, pronounced changes in the pEDMR spectra may be observed. Due to the fact that pEDMR allows a deconvolution of the spin-dependent signals in time as well as in magnetic field domain, we were able to significantly reduce the complexity of the spectra compared to conventional EDMR. In the samples containing amorphous n-type contact layers we found signals from shallow localized conduction band tail states and phosphorous donor states. Upon replacement of this layer by its microcrystalline counterpart both signals disappeared. Possible spin-dependent transport mechanisms involving paramagnetic states in the various layers are discussed in view of sign and time evolution of the associated pEDMR signals.     

Low-cost high-temperature NMR probe head

The design of a simple high-temperature nuclear magnetic resonance (NMR) probe head for narrow-bore magnets is presented. It covers the temperature range from 20 to 1300°C, necessitating a heating power of below 100 W. Several probe heads of this design, manufactured for NMR solenoids with bores from 30 to 54 mm have shown good stability and long life times.