Anisotropic rotations in 1-naphthylamine. Existence of a red-edge transition moment normal to the ring plane

The rotational motions of 1-naphthylamine in propylene glycol are investigated by means of steady-state flourescence polarization measurements and differential polarized phase flourometry, on excitation at various wavelengths. For excitation at 370 nm the average rotational rate is faster than for excitation at shorter wavelength and the rotations are clearly anisotropic. On excitation from 370nm to the red edge of the spectrum (390 nm) the average rotational rate slows down by a factor of two and the rotations become nearly isotropic. The results reveal the possible existence of an excited state generated preferentially by excitation at the edge of the absorption, in which the transition moments in both absorption and emission are prependicular to the plane of the aromatic rings.     

A possible interaction between gravity and the electric field

A charged parallel plate capacitor contains less electric energy when its plates are oriented parallel to a gravitational field than it contains when its plates are oriented perpendicular to the same field. If this energy difference can be detected by an observer located inside the field, then the capacitor should experience a torque until the electric field is perpendicular to the radial direction.     

Synthese und Struktur hochfunktionalisierter 2, 3‐Dihydro‐1H‐1, 3, 2‐diazaborole

Synthesis and Structure of Highly Functionalized 2, 3‐Dihydro‐1H‐1, 3, 2‐diazaboroles A series of differently substituted 2, 3‐dihydro‐1H‐1, 3, 2‐diazaboroles has been prepared by various methods. 1, 3‐Di‐tert‐butyl‐2‐trimethylsilylmethyl‐1H‐1, 3, 2‐diazaborole ( 7 ), 2‐isobutyl‐1, 3‐bis(1‐cyclohexylethyl)‐1H‐1, 3, 2‐diazaborole ( 8 ), 1, 3‐bis‐(1‐cyclohexylethyl)‐2‐trimethylsilylmethyl‐1H‐1, 3, 2‐diazaborole ( 9 ) 1, 3‐bis(1‐methyl‐1‐phenyl‐propyl)‐2‐trimethylsilylmethyl‐1H‐1, 3, 2diazaborole ( 10 ) and 2‐bromo‐1, 3‐bis(1‐methyl‐1‐phenyl‐propyl)‐1H‐1, 3, 2‐diazaborole ( 11 ) were formed by reaction of the corresponding 1, 4‐diazabutadienes with the boranes Me₃SiCH₂BBr₂, iBuBBr₂ and BBr₃ followed by reduction of the resulting borolium salts [R¹ = tBu, Me(cHex)CH, [Me(Et)Ph]C; R² = Me₃SiCH₂, iBu, Br] with sodium amalgam. Treatment of 11 and 12 with silver cyanide afforded the 2‐cyano‐1, 3, 2‐diazaboroles 13 and 14 . An alternative route to compound 8 is based on the alkylation of 2‐bromo‐1, 3, 2‐diazaborole 12 with isobutyllithium. Equimolar amounts of 13 and isobutyllithium give rise to the formation of 15 . The new compounds were characterized by ¹H‐, ¹³C‐, ¹¹B‐NMR, IR and mass spectra. The molecular structures of 7 and meso ‐10 were confirmed by x‐ray structural analysis.     

Charge effects during surface analysis of poorly conducting inorganic materials

Summary The properties of surfaces and interfaces often determine the behaviour of materials in a given application: typical examples are all kinds of corrosion, segregation, sensor activity, wear and friction, adhesion of coatings, joining processes, sintering, etc. It is the aim of this paper to provide materials scientists with a better understanding of the limits of applying modern surface analysis methods (SIMS, AES, etc.) to materials with low room temperature electrical conductivity like most ceramics and glasses. One feature common to all methods deserves special attention: this is the influence of surface and near surface charges on the distribution of mobile ionic species in the near surface region of the sample to be analyzed. The origin of these charges and their order of magnitude as a function of the experimental parameters can be deduced from charge balance considerations: the main result is that self-compensating methods should be most favorable.     

Hadronic equation of state and the onset of kaon condensation

An equation of state is presented which takes the finite size of baryons and of mesons consistently into account and incorporates the contributions of both nonstrange and strange hadrons. All extensive quantities (energy, particle number, entropy) are modified by a factor taking into account the excluded volume due to baryon repulsion. Intensive quantities (pressure) are not modified. This is achieved by introducing a baryon chemical potential, _B, which is shifted from its point-like value, _B ⁰ , by a term proportional to the finite volume of a hadron,V ₀, as follows: _B= _B ⁰ + V₀[P⁰(T, _B ⁰ )–P⁰(T, 0)], whereP ⁰ is the pressure for pointlike particles. The last term is necessary to conserve baryon number at the phase transition point. The differences between the new equation of state and those considered previously in the literature are discussed. It is shown that kaon condensation sets in only in the mixed phase of the transition, where hadrons, quarks and gluons are present simultaneously in thermodynamical equilibrium.     

Dynamical and thermal aspects of relativistic heavy-ion collisions

Within a covariant BUU-approach we simulate heavyion collisions at various bombarding energies from 400 MeV/u to 1 GeV/u. We evaluate locally the energymomentum tensorT ^v (x), and extract pressures, energydensities and temperatures. The connection of these thermodynamical quantities to experimental observables and their sensitivity to the equation of state is discussed. Furthermore, we investigate the question of local equilibration and evaluate the entropy produced in these reactions.Dedicated to Prof. Dr. P. Kienle on the occasion of his 60th birthday. Work supported by BMFT and GSI Darmstadt