Integrating DEA-oriented performance assessment and target setting using interactive MOLP methods

Data envelopment analysis (DEA) and multiple objective linear programming (MOLP) are tools that can be used in management control and planning. Whilst these two types of model are similar in structure, DEA is directed to assessing past performances as part of management control function and MOLP to planning future performance targets. This paper is devoted to investigating equivalence models and interactive tradeoff analysis procedures in MOLP, such that DEA-oriented performance assessment and target setting can be integrated in a way that the decision makers’ preferences can be taken into account in an interactive fashion. Three equivalence models are investigated between the output-oriented dual DEA model and the minimax reference point formulations, namely the super-ideal point model, the ideal point model and the shortest distance model. These models can be used to support efficiency analysis in the same way as the conventional DEA model does and also support tradeoff analysis for setting target values by individuals or groups. A case study is conducted to illustrate how DEA-oriented efficiency analysis can be conducted using the MOLP methods and how such performance assessment can be integrated into an interactive procedure for setting realistic target values.     

H-D exchange on graphite-potassium intercalation compounds

Potassium graphite intercalation compounds are able to activate C-H bonds of hydrocarbons at room temperature. In this paper, the hydrogen-deuterium exchange of CHD(3) in the presence of C(8)K, C(24)K and C(36)K is described.     

Kinetic studies for the esterification of acetic acid with epichlorohydrin over an anion exchange resin catalyst

The kinetics of the esterification reaction between acetic acid and epichlorohydrin catalysed by Purolite A-520E strong basic anion exchange resin was studied. The effects of certain parameters such as stirring speed, particle diameter, temperature, catalyst amount and molar ratio between reactants were experimentally determined. It was found that the overall reaction rate is intrinsically kinetically controlled. The partial orders of reaction with respect to catalyst, acetic acid and epichlorohydrin were determined. A reaction mechanism is proposed. Based on chromatographic data and taking into account the partial orders of reaction, a more detailed kinetic model is suggested.      

Development and validation of an LC‐ESI‐MS/MS quantification method for a potential γ‐aminobutyric acid transporter 3 (GAT3) marker and its application in preliminary MS binding assays

Binding assays for the γ‐aminobutyric acid (GABA) transporter GAT3 can be assumed to significantly facilitate screening for respective inhibitors. As appropriate labeled ligands for this promising drug target are not available so far, we started efforts to set up mass spectrometry‐based binding assays (MS binding assays), for which labeled markers are not required. Therefore, we developed a sensitive and rapid LC‐ESI‐MS/MS quantification method for DDPM‐1007 {(RS)‐1‐[4,4,4‐Tris(4‐methoxyphenyl)but‐2‐en‐1‐yl]piperidine‐3‐carboxylic acid}, one of the most potent GAT3 inhibitors yet known, as a potential GAT3 marker. Using a 50 × 2 mm C₈ column in combination with a mobile phase composed of 10 mm ammonium bicarbonate buffer pH 8.0 and acetonitrile (60:40, v/v) at a flow rate of 450 μL/min DDPM‐1007 could be analyzed in the positive multiple reaction monitoring mode [(m/z) 502.5 → 265.4] within a chromatographic cycle time of 3 min. Deuterated DDPM‐1007 [(²H₉)DDPM‐1007] was synthesized and employed as internal standard. This way DDPM‐1007 could be quantified in a range from 100 pm to10 nm in the matrix resulting from respective binding experiments without any sample preparation. The established quantification method met the requirements of the FDA guidance for bioanalytical method validation concerning linearity and intra‐ and inter‐batch accuracy. Based on this LC‐ESI‐MS/MS quantification preliminary MS binding assays employing membrane preparations obtained from a stably GAT3 expressing HEK293 cell line and DDPM‐1007 as nonlabeled GAT3 marker could be performed. In these experiments specific binding of DDPM‐1007 at GAT3 could be unambiguously detected. Additionally, the established LC‐MS method provides a suitable analytical tool for further pharmacokinetic characterization of DDPM‐1007, as exemplified for its logD determination. Copyright © 2012 John Wiley & Sons, Ltd.     

Slow Inversion of Coordinated Thioether Groups in SNS-Type Ruthenium Pincer Complexes

The thioether-group-containing SNS-type pincer complex [({EtSCH₂CH₂}₂NH)RuCl(H)(PPh₃)] ( 2 ) exists in three different diastereomers ( 2 a – c ). The molecular structures obtained from single crystal X-Ray diffraction studies of all three isomers reveal a difference in the relative orientation of the respective EtS-groups, while other commonly observed diastereomers as the result of cis-/trans- or fac-/mer-isomerism are not observed. Chemical exchange between the three diastereomers 2 a – c was discovered by phase-sensitive ¹H and ³¹P NOESY NMR spectroscopy, and further quantified by line shape analysis of ¹H NMR spectra. The experimentally derived averaged Gibbs energies of activation for the interconversion of the isomers (65–70 kJ/mol) are in good agreement with the results obtained from DFT calculations, which suggest an inversion of the ligating sulfur atoms, although a dissociative pathway for the configurational inversion can be competitive.     

Few‐cycle,broadband, mid‐infrared optical parametric oscillator pumped by a 20‐fs Ti:sapphire laser

A few‐cycle, broadband, singly‐resonant optical parametric oscillator (OPO) for the mid‐infrared based on MgO‐doped periodically‐poled LiNbO₃ (MgO:PPLN), synchronously pumped by a 20‐fs Ti:sapphire laser is reported. By using crystal interaction lengths as short as 250 µm, and careful dispersion management of input pump pulses and the OPO resonator, near‐transform‐limited, few‐cycle idler pulses tunable across the mid‐infrared have been generated, with as few as 3.7 optical cycles at 2682 nm. The OPO can be continuously tuned over 2179‐3732 nm (4589‐2680 cm^‐1) by cavity delay tuning, providing up to 33 mW of output power at 3723 nm. The idler spectra exhibit stable broadband profiles with bandwidths spanning over 422 nm (FWHM) recorded at 3732 nm. The effect of crystal length on spectral bandwidth and pulse duration is investigated at a fixed wavelength, confirming near‐transform‐limited idler pulses for all grating interaction lengths. By locking the repetition frequency of the pump laser to a radio‐frequency reference, and without active stabilization of the OPO cavity length, an idler power stability better than 1.6% rms over >2.75 hours is obtained when operating at maximum output power, in excellent spatial beam quality with TEM₀₀ mode profile. Photograph shows a multigrating MgO:PPLN crystal used as a nonlinear gain medium in the few‐cycle femtosecond mid‐IR OPO. The visible light is the result of non‐phase‐matched sum‐frequency mixing between the interacting beams.     

Volume and grain boundary diffusion of implanted 113Sn in aluminium

Volume and grain boundary diffusion of ¹¹³Sn in aluminium was investigated with the radiotracer method. The implantation technique was used for tracer deposition to avoid problems of tracer hold-up caused by the oxide layer always present on aluminium. The diffusion penetration was chosen large enough to permit serial sectioning of samples with the aid of a microtome.The temperature dependence of the volume diffusivity was determined as D(T)=4.54×10^–5×exp[–(114.5±1.2)kJmol^–1/RT] m ² s ^–1. This confirms previous measurements from our group which already showed that Sn is the fastest foreign metal diffusor so far investigated in aluminium.Grain boundary diffusion of ¹¹³Sn in Al polycrystals was measured in the type-B kinetic regime. The grain boundary diffusion product P=sD _gb (s=segregation factor, =grain boundary width, D _gb=grain boundary diffusivity) was found to be strongly affected by the impurity content of aluminium. For Al polycrystals of 99.9992% nominal purity we obtained P _5N(T)=1.08×10^–8exp [–(96.9±7.5) kJ mol^–1/RT] m³ s^–1 and for less pure Al polycrystals of 99.99% nominal purity P _4N(T)=3.0×10^–10 exp [–(90.1±4.2) kJ mol^–1/RT] m³ s^–1 was determined. The grain boundary diffusion product in the purer material is more than one order of magnitude higher than in the less pure material. Very likely this is an effect of co-segregation of non-diffusant impurities into the grain boundaries.