Total and free endotoxin release in time from cultures of Escherichia coli by different antibiotics was studied in vitro for 4 h in relation to the antibiotic effect on viable counts and morphological features of the test cultures. The most rapid fall in viable counts was seen after treatment with imipenem or the combination of imipenem with tobramycin, accompanied by an early, but minimal increase (1.8-fold) of the total (free plus cell-bound) endotoxin level at 1 h. Total endotoxin levels increased approximately 5-fold upon incubation with ceftazidime, tobramycin or the combination of tobramycin with cefuroxime, whereas incubation with cefuroxime or aztreonam alone caused a late 22-and 49-fold increase in total endotoxin, respectively, at 4 h. In chloramphenicol treated cultures there was still an increase in viable counts during therapy, resulting in an ultimately 78-fold increase of mean levels of total endotoxin. Free endotoxin levels increased approximately 6-fold within 1 h upon treatment with imipenem, alone or in combination with tobramycin, or ceftazidime as the result of rapid lysis of bacteria. Treatment with cefuroxime or aztreonam induced a relatively late but much higher release of free endotoxin (118-and 222-fold, respectively), which was due to the formation of long filamentous structures during the first 2 h of incubation and eventually cell lysis. Both tobramycin and the combination of tobramycin with cefuroxime caused a more gradual rise in free endotoxin, with a +/- 15-fold increase in free endotoxin at 4 h. In chloramphenicol treated cultures, as in the control cultures, the level of free endotoxin remained proportional to the amount of viable organisms. We also studied plasma endotoxin levels in 20 patients with septic shock. 10 out of these 20 patients had a detectable endotoxemia (greater than 5 ng/l) on admission. We describe the patterns of plasma endotoxin in these patients during the first 24 h of antibiotic treatment. We conclude that, in the in-vitro study, values of total endotoxin, free endotoxin, and the rate of release of endotoxin varies with the antibiotic used. We also demonstrate that in patients under treatment for septic shock endotoxin release can be related to the administration of antibiotics.

Energy spectra of electrons resulting from collisions of bare ions C +H2 and O' +He are presented. A detailed analysis is given for those parts of the spectra that are due to two-electron capture into (31, 31') configurations of the He-like projectile ions and subsequent autoionization.Measured peaks are uniquely identified by comparison with existing theoretical calculations. Based on a detailed investigation, it is concluded that an influence of interference effects on the spectra cannot be identified. A quantitative fit of the spectra allows us to determine the population probabilities of the various states with (31, 31') configuration. We find a preferential population of states that can be characterized by a correlated electronic motion with the two electrons on opposite sides of the capturing ion and rotating in the same sense. This result is discussed in terms of a classical picture for the capturing process.

A semiclassical theory is applied to describe collisions between sodium atoms which are independently excited to a specific magnetic sublevel of the 3p state. Cross sections for energy transfer are calculated for different combinations of the initial magnetic quantum numbers (ma,mb) of the atoms, and as a function of the thermal collision velocity. The motion of the cores is described either by curved trajectories, based on non-averaged adiabatic potential curves, or by straight trajectories. The largest basis set used for the electronic wavefunction contains the 4p, 5s, 4d and 4f exit channels. The electronic interaction Hamiltonian is approximated by a multipole expansion, for which all non-vanishing contributions are evaluated.

In a beam experiment the authors have studied the energy pooling reaction between two laser excited Na* (3p) atoms, where in the final state one of the sodium atoms is in the 5s or 4d state and the other in the ground state. They have determined all eight independent partial cross sections and coherence terms, specified according to the various magnetic substate combinations of the colliding Na* (3p) atoms, as a function of the collision velocity. This is the maximum information that can be extracted from the experiment given the symmetry of the detection scheme. By applying a weak magnetic field, to orient the Na* (3p) atoms, the authors were able to distinguish between the two partial cross sections sigma 11 and sigma 1-1, where the subscripts 11 and 1-1 refer to the initial magnetic substate combinations of the two collision partners. By using an electro-optical modulator the authors have furthermore improved the signal-to-noise ratio to an extent where it was possible to measure all coherence terms.

The authors have studied, in a beam experiment, the energy pooling reaction between two laser excited Na*(3p) atoms, where in the final state one of the Na atoms is in the 5s or 4d state and the other in the ground state. The polarization of the Na*(3p) atoms can be varied by changing the laser polarization. By using two counterpropagating Na beams and intersecting them twice by a laser beam (directly and indirectly after reflection against a mirror) the polarization of the two collision partners can be varied independently. Since the laser beam intersects the Na beams at an angle of 87.6 degrees , the relative velocity of the atoms can furthermore be selected by exploiting the Doppler effect. In the authors' experiment the relevant cross sections and coherences, specified according to the various magnetic substate combinations of the colliding Na*(3p) atoms, can be determined.