Perfluormethyl‐Element‐Liganden. XLIII [1] Neue Synthesewege zu Zweikernkomplexen des Typs MM′(CO)8ER2X (M/M′ = Mn/Mn,Mn/Re,Re/Re; E = P,As; R = CF3, Me; X = Hal)

Perfluoromethyl Element Ligands. XLIII [1] Novel Synthetic Routes to Binuclear Complexes of the Type MM′(CO)₈ER₂X (M/M′ = Mn/Mn, Mn/Re, Re/Re; E = P, As; R = CF₃, Me; X = Hal, ) Mn(CO)₅I reacts with compounds of the type (CF₃)₂EAsMe₂ (E = P, As) as with the symmetric E₂(CF₃)₄ ligands in the first step with cleavage of the E‐As bond to yield the pro ducts (CO)₅MnE(CF₃)₂ and Me₂AsI. Reaction of the mononuclear complexes with excess of Mn(CO)₅I leads in good yields to the known dinuclear compounds (CO)₄Mn[E(CF₃)₂, I]Mn(CO)₄ and CO. Me₂AsI, the second product of the EAs cleavage, attacks the starting compound Mn(CO)₅I giving cis‐Mn(CO)₄I(AsMe₂I) and CO. This result encouraged us to thoroughly investigate the preparation of cis‐M(CO)₄X(EMe₂Y) complexes with most of the possible combinations of M = Mn, Re; E = P, As and X, Y = Cl, Br, I. An alternative route to these compounds was opened by the cleavage of the dinuclear manganese or rhenium halides M₂(CO)₈X₂ with the halophosphanes or ‐arsanes Me₂EY. This route was found to be especially advantageous for the preparation of the rheniumcarbonyl precursors, since milder conditions than for the CO‐substitution in Re(CO)₅X compounds are sufficient for the halogen‐bridged dinuclear complexes. Cis‐M(CO)₄X(EMe₂Y) complexes were used as precursors for the synthesis of novel homo‐ and heterodinuclear complexes of the type (CO)₄M(EMe₂, X)M′(CO)₄ by reacting the EY function with transition metal carbonylates Kat[M′(CO)₅] (Kat = Na, Bu₄N, Ph₄As). Thus the preparation of a wide range of complexes was possible, which before had been successfully prepared by the direct reaction of Mn₂(CO)₁₀ with Me₂EX only in few cases, e. g. with Me₂AsI. Spectroscopic investigations, using the CO valence frequencies and the ¹H‐NMR data of the ligands EMe₂Y or of the Me₂E bridges, were applied to study the influence of the variables M, M′, E, X, Y and Kat on the reactivity of the mononuclear complexes and the bonding situation in both the mono‐ and the dinuclear systems. The new compounds were characterized by spectroscopic (IR, NMR, MS) and analytic methods (C, H).     

Optoacoustic sensor head for depth profiling

-1 (for 0.25 mJ/cm²). The response function of the total experimental setup is derived from the optoacoustic signal of a black absorber, which is necessary to correct theoretical calculations with regard to the finite time response of the detection system. In the case of homogeneous samples, the theory of optoacoustic signal generation is verified, qualitative results are achieved with layered samples. Received: 14 October 1998 / Published online: 24 February 1999     

Design and fabrication of electrospun polyethersulfone nanofibrous scaffold for high‐flux nanofiltration membranes

A novel class of high‐flux and low‐fouling thin‐film nanofibrous composite (TFNC) membranes, containing a thin hydrophilic top‐layer coating, a nanofibrous mid‐layer scaffold and a non‐woven microfibrous support, has been demonstrated for nanofiltration (NF) applications. In this study, the issues related to the design and fabrication of a polyethersulfone (PES) electrospun nanofibrous scaffold for TFNC NF membranes were investigated. These issues included the influence of solvent mixture ratio, solute concentration, additives, relative humidity (RH), and solution flow rate on the morphology of an electrospun PES nanofibrous scaffold, the distribution of fiber diameter, the adhesion between the PES scaffold and a typical poly(ethylene terephthalate) (PET) non‐woven support, as well as the tensile properties of the nanofibrous PES/non‐woven PET composite substrates. Uniform and thin nanofibrous PES scaffolds with strong adhesion to the nanofiber‐PET non‐woven are several of the key parameters to optimize the NF performance of TFNC membranes. © 2009 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 47: 2288–2300, 2009     

Zur Erkennung und quantitativen Bestimmung von salpetriger S?ure oder Salpeters?ure in k?uflicher Schwefels?ure

Ohne Zusammenfassung     

Auf eine Methode zur spectralanalytischen Untersuchung der Resorcinfarbstoffe

Ohne Zusammenfassung     

Observation of B --> K(+/-) pi(0) and B --> (K)0 pi(0), and evidence for B --> pi(+)pi(-)

We have studied charmless hadronic decays of B mesons into two-body final states with kaons and pions and observe three new processes with the following branching fractions: beta(B-->pi(+)pi(-)) = (4.3(+1. 6)(-1.4)+/-0.5)x10(-6), beta(B-->K(0)pi(0)) = (14.6(+5.9+2.4)(-5.1-3. 3))x10(-6), and beta(B-->K(+)/-pi(0)) = (11.6(+3.0+1.4)(-2.7-1.3))x10(-6). We also update our previous measurements for the decays B-->K(+)/-pi(-/+) and B+/--->K(0)pi(+/-).     

Two-body B meson decays to eta and eta('): observation of B --> eta K*

In a sample of 19 x 10(6) produced B mesons, we have observed the decays B-->eta K(*) and improved our previous measurements of B-->eta'K. The branching fractions we measure for these decay modes are B(B+-->eta K(*+)) = (26.4(+9.6)(-8.2)+/-3.3)x10(-6), B(B(0)-->eta K(*0)) = (13.8(+5.5)(-4.6)+/-1.6)x10(-6), B(B(+)-->eta'K(+) = (80(+10)(-9)+/-7)x10(-6), and B(B(0)-->eta'K0) = (89(+18)(-16)+/-9)x10(-6). We have searched with comparable sensitivity for related decays and report upper limits for these branching fractions.