Stereoisomers of N-[1-hydroxy-(2-phenylethyl)-3-methyl-4-piperidyl]- N-phenylpropanamide: synthesis, stereochemistry, analgesic activity, and opioid receptor binding characteristics

N-[1-(2-Hydroxy-2-phenylethyl)-3-methyl-4-piperidyl]-N-phenylpropanamide (ohmefentanyl,1) is an extremely potent analgesic agent with high affinity and selectivity for opioid mu receptors. There are three chiral carbons in 1, so eight optically active isomers are possible. Respective reaction of optically active 3-methyl-N-phenyl-4 -piperidinamines (5a-d) with (R)- or (S)-styrene oxide produced eight optically active intermediates which were subsequently converted to eight optically active isomers of 1 (1a-h). The absolute configurations of 1a-h were determined by X-ray analysis of (3R,4S,2'R)-(-)-cis-1a and (3R,4R,2'S)-(-)-trans-1g. The analgesic activity (mice, ip, hot plate) revealed their extreme stereodifferences; the ED50 values of (3R,4S,2'R)-(-)-cis-1a and (3R,4S,2'S)-(+)-cis-1b, which are the most potent isomers among eight isomers, were 0.004 65 (2990 times that of morphine) and 0.001 06 mg/kg (13 100 times that of morphine), respectively, while the corresponding antipodes 1d,c were the least potent compounds among the eight isomers. In agreement with pharmacological results, both 1a,b also had the highest receptor affinity and selectivity for the opioid mu receptor. The ratio of K(i)(DPDPE)&K(i)(DAMGO) was 22 800 for 1a and 22 500 for 1b. All isomers except 1c,d strongly inhibited the electrically evoked smooth muscle contraction of GPI and MVD but not that of RVD, and the inhibitory effects could be reversed by naloxone, which indicated that these compounds were potent mu agonists in GPI and MVD. There was a good linear correlation between the analgesic potencies (ED50) and the receptor affinities (K(i)(DAMGO)) or inhibitory effects (IC50) to GPI and MVD. These results suggested that the analgesic effects of ohmefentanyl are mediated by interaction between the agents and opioid mu receptors in the central nervous system and the 3R,4S configuration at the piperidine 3- and 4-carbon atoms and the S configuration at the phenylethyl 2-carbon atom are beneficial for analgesic potency and inhibitory effects in GPI and MVD and the same for an S or R configuration at the phenylethyl 2-carbon atom besides the 3R,4S configuration for receptor mu affinity and selectivity.     

Formation of TiSi2 and shallow junction byAs+ ion-beam mixing and infrared rapid heat treatment

A technique for forming shallow junctions with low-resistance silicide contacts developed for the use in VLSI with scaled MOSFETs is discussed. The salicide (self-aligned silicide) MOSFET gate and source-drain features self-aligned refractory metal silicide and are isolated from one another even without any insulating spacer on the gate sides. A critical step in such a MOSFET fabrication process is the ion implantation through metal silicidation technique, which includes As⁺ ion-beam-induced titanium-silicon interface mixing and infrared rapid heat treatment to form simultaneously the n⁺-p junction and a high-quality TiN covered TiSi₂ contact layer     

The elusive ettringite under the high‐vacuum SEM – a reflection based on natural samples,the use of Monte Carlo modelling of EDS analyses and an extension to the ettringite group minerals

Ettringite, Ca₆Al₂(SO₄)₃(OH)₁₂.26H₂O, or C₆A₃H₃₂ as it is known in cement chemistry notation, is a major phase of interest in cement science as an hydration product and in polluted soil treatment since its structure can accommodate with many hazardous cations. Beyond those anthropogenic features, ettringite is first of all a naturally occurring mineral (although rare). An example of its behaviour under the scanning electron microscope and during energy dispersive spectroscopy (EDS) qualitative analysis is presented, based on the study of natural ettringite crystals from the N'Chwaning mine in South Africa. Monte Carlo modelling of the electron‐matter interaction zone at various voltages is presented and confronted with actual, observed beam damage on crystals, which burst at the analysis spot. Finally, theoretical energy dispersive spectroscopy spectra for all the ettringite group minerals have been computed as well as Monte Carlo modelling of the electron‐matter interaction zone. The knowledge of the estimation of the size of this zone may thus be helpful for the understanding of energy dispersive spectroscopy analysis in cement pastes or ettringite‐remediated soils.