Production of HD Molecules in Definite Hyperfine Substates.

Polarized atomic beam sources have been in operation for many years to produce either nuclear polarized atomic hydrogen or deuterium beams. In recent experiments, such a source was used to polarize both isotopes independently at the same time. By recombination of the atoms, hydrogen-deuterium molecules with all possible nuclear spin combinations can be created. Those spin isomers are useful for further applications, like precision spectroscopy, as polarized targets for laser-particle acceleration, polarized fuel for fusion reactors, or as an option for future measurements of electric dipole moments.

Isotensor Dibaryon in the pp→ppπ

Exclusive measurements of the quasifree pp→ppπ^{+}π^{-} reaction have been carried out at WASA@COSY by means of pd collisions at T_{p}=1.2 GeV. Total and differential cross sections have been extracted covering the energy region T_{p}=1.08-1.36 GeV, which is the region of N^{*}(1440) and Δ(1232)Δ(1232) resonance excitations. Calculations describing these excitations by t-channel meson exchange are at variance with the measured differential cross sections and underpredict substantially the experimental total cross section. An isotensor ΔN dibaryon resonance with I(J^{P})=2(1^{+}) produced associatedly with a pion is able to overcome these deficiencies.

Spin Dependence of η Meson Production in Proton-Proton Collisions Close to Threshold.

Taking advantage of the high acceptance and axial symmetry of the WASA-at-COSY detector, and the high polarization degree of the proton beam of COSY, the reaction p[over →]p→ppη has been measured close to threshold to explore the analyzing power A_{y}. The angular distribution of A_{y} is determined with the precision improved by more than 1 order of magnitude with respect to previous results, allowing a first accurate comparison with theoretical predictions. The determined analyzing power is consistent with zero for an excess energy of Q=15 MeV, signaling s-wave production with no evidence for higher partial waves. At Q=72 MeV the data reveal strong interference of Ps and Pp partial waves and cancellation of (Pp)^{2} and Ss^{*}Sd contributions. These results rule out the presently available theoretical predictions for the production mechanism of the η meson.

Abashian-Booth-Crowe effect in basic double-pionic fusion: a new resonance?

We report on an exclusive and kinematically complete high-statistics measurement of the basic double-pionic fusion reaction pn→dπ(0)π(0) over the full energy region of the ABC effect, a pronounced low-mass enhancement in the ππ-invariant mass spectrum. The measurements, which cover also the transition region to the conventional t-channel ΔΔ process, were performed with the upgraded WASA detector setup at COSY. The data reveal the Abashian-Booth-Crowe effect to be uniquely correlated with a Lorentzian energy dependence in the integral cross section. The observables are consistent with a narrow resonance with m=2.37 GeV, Γ≈70 MeV and I(J(P))=0(3(+)) in both pn and ΔΔ systems. Necessary further tests of the resonance interpretation are discussed.

Polarized proton acceleration in ultraintense laser interaction with near-critical-density plasmas.

The production of polarized proton beams with multi-GeV energies in ultraintense laser interaction with targets is studied with three-dimensional particle-in-cell simulations. A near-critical density plasma target with prepolarized proton and tritium ions is considered for the proton acceleration. The prepolarized protons are initially accelerated by laser radiation pressure before injection and further acceleration in a bubblelike wakefield. The temporal dynamics of proton polarization is tracked via the Thomas-Bargmann-Michel-Telegdi equation and it is found that the proton polarization state can be altered by both the laser field and the magnetic component of the wakefield. The dependence of the proton acceleration and polarization on the ratio of the ion species is determined and it is found that the protons can be efficiently accelerated as long as their relative fraction is less than 20%, in which case the bubble size is large enough for the protons to obtain sufficient energy to overcome the bubble injection threshold.

Nm-sized cryogenic hydrogen clusters for a laser-driven proton source.

A cryogenic hydrogen cluster-jet target is described which has been used for laser-plasma interaction studies. Major advantages of the cluster-jet are, on the one hand, the compatibility to pulsed high repetition lasers as the target is operated continuously and, on the other hand, the absence of target debris. The cluster-jet target was characterized using the Mie-scattering technique allowing to determine the cluster size and to compare the measurements with an empirical formula. In addition, an estimation of the cluster beam density was performed. The system was implemented at the high power laser system ARCTURUS, and the measurements show the acceleration of protons after irradiation of the cluster target by high intensity laser pulses with a repetition rate of 5 Hz.

Activation of the c-fos gene by UV and phorbol ester: different signal transduction pathways converge to the same enhancer element.

In NIH3T3 cells stably transfected with the human c-fos gene, serum, platelet derived growth factor (PDGF), phorbol ester (12-O-tetradecanoyl-phorbol-13-acetate, TPA), ultraviolet irradiation (UV) and 3'-5'-cyclic adenosine monophosphate (cAMP) cause a transient and rapid activation of both the endogenous and the transfected c-fos genes. While serum, TPA, UV and PDGF dependent activation of the gene is severely impaired, when the serum responsive element from position -319 to -300 (SRE, Treisman, 1985) is destroyed, a full response to cAMP is retained. Insertion of a synthetic oligonucleotide corresponding to the SRE element upstream of position -96 restores the responses to TPA and serum, and large parts of the responses to UV and PDGF. The signal transduction chains elicited by UV and TPA are blocked by an inhibitor of protein kinase. Only TPA, however, causes the translocation of protein kinase C to the membrane. UV and TPA treated cells become refractory to a second stimulation by the same agent at 3 or 24 hours after the first treatment. Alternating the agents, however, leads to full responses. In addition, saturating doses of UV and TPA are at least additive. Ca-ionophores severely reduce only UV induced c-fos expression. These data indicate, that different signal transduction pathways elicited by growth promoting agents and by UV induced stress converge onto the same enhancer element.

The Fos and Jun/AP-1 proteins are involved in the downregulation of Fos transcription.

The low basal expression of Fos and the rapid and effective turn-off of serum induced Fos transcription is due to autoregulation. Fos and Jun/AP-1 protein cooperate in the repression mechanism. Overexpressions of Fos and Jun decrease basal and induced transcription from Fos-CAT constructs and from the endogenous gene in NIH3T3 cells. The introduction into cells of either antisense Fos or antisense Jun sequences leads to elevated basal Fos promoter activity. Gel retardation experiments with synthetic oligonucleotides define two target sequences in the Fos promoter which bind Fos-Jun/AP-1 (centering at about -296 and -60). In vivo competition with these oligonucleotides relieves repression.

Evolution of placenta-specific gene expression: comparison of the equine and human gonadotropin alpha-subunit genes.

Primate and equine species are thought to be unique among mammals in synthesizing placental gonadotropin glycoprotein hormones. Human chorionic gonadotropin (CG) and equine pregnant mare's serum gonadotropin (PMSG) are produced in placenta by the specific activation of a glycoprotein hormone alpha-subunit gene and a corresponding beta-subunit gene. The evolutionary mechanisms for the apparently independent acquisition of tissue specificity were investigated by cloning the 5' flanking region of the equine alpha-subunit gene and comparing the DNA elements and trans-acting factors involved in placental expression. We find that though the equine gene is expressed and induced by cAMP, it does not contain the elements known to confer tissue-specific expression to the human gene, the cAMP response element (CRE) and the trophoblast-specific element (TSE), nor does it bind to the trans-acting factors CREB and TSEB. Instead, an additional factor (alpha-ACT) is found which binds to the equine and human, but not the murine, alpha-subunit genes in a region between the positions of the CRE and TSE and confers cAMP responsiveness.

Coordinate control of the alpha- and beta-subunit genes of human chorionic gonadotropin by trophoblast-specific element-binding protein.

The alpha- and beta-subunit genes of hCG are coordinately regulated in the trophectoderm of the early embryo and placenta. Placenta-specific expression of the alpha-subunit gene is determined by a composite enhancer made of three clustered components: cAMP-responsive elements, a GATA site, and the trophoblast-specific element (TSE). We have investigated the basis of placenta-specific expression of the major hCG beta-subunit gene, hCG beta 5. Enhancement of expression localizes to the region from -305 to -279, whereas full cAMP regulation requires the region from -305 to -249. Four DNAse-I footprints are present, three of which can be competed by the TSE element from the alpha-subunit gene. Methylation interference establishes that binding to the element located in the key region for expression, from -301 to -275, requires contacts with a CCNNNGGG core sequence that matches the alpha-subunit gene TSE. Sequence-specific DNA affinity chromatography using the alpha-subunit gene TSE allows purification of TSE-binding protein. This purified protein binds specifically to the key element, -301 to -275, and to at least two additional TSE elements clustered in the regulatory region of the hCG beta 5 gene. We conclude that both the alpha- and beta-subunit genes of hCG require the placenta-specific factor TSE-binding protein for expression, providing a mechanism for their coordinate regulation in placental cells.

Peroneal nerve neuropathy in cancer patients: a paraneoplastic syndrome?

AIMS: To investigate the occurrence of symptomatic peroneal neuropathy (PN) in cancer patients, as well as that of cancer in PN patients and to seek possible factors in the aetiology of PN. METHODS: Clinical, neurographical, and myographical data of patients with PN, in two general neurology clinics during a 5-year period (1988-1992) were analysed retrospectively. A population-based cancer registry was consulted for epidemiological data in the area. RESULTS: The catchment population of the two clinics consisted of 433,142 people, and 8,766 new cancer patients were diagnosed. PN was diagnosed in 372 patients, of whom 74 suffered from cancer (in 56 PN was believed to be related to cancer). The crude relative risk of PN in patients with cancer compared with patients without cancer was 8.6. After correction for differences in age and sex between the compared groups, the relative risk dropped to 3.4 (2.8 for women and 3.6 for men). The crude relative risk of cancer for patients with PN relative to people without PN was 7.5. The relative risk, after correction for age and sex, was 2.8 (2.5 for women and 2.9 for men). All relative risks were significant (P < 0.001), but did not differ between the sexes (P > 0.4). Weight loss was established in 35/56 patients, but in 17/56 it was unknown. PN has not been found to be part of a polyneuropathy. Chemotherapy did not play a causal part. In some patients PN preceded the diagnosis of cancer. CONCLUSIONS: The occurrence of PN seems to be higher in patients with cancer than in people without cancer. Cancer was found in patients with PN more often, particularly in elderly men, than would be expected from the occurrence in the total population. PN in patients with cancer is supposed to be due to a combination of metabolic and mechanical factors. The findings justify a prospective study of the relation between PN and cancer.

A modification of the HS3 thoracic Alpha Cradle for breast/chestwall patients.

The problem of the sloping chest wall in tangential irradiation of the breast or chest wall is solved by a unique modification of the Smithers HS3 thoracic immobilizer. The need for a cumbersome angled breast board or collimator rotation is eliminated.

The building of free-form customized immobilizers.

Unusual immobilization problems occur in radiation therapy. A solution using styrofoam sheet and blocks, mylar sheet and urethane foaming chemicals is suggested here. The technique is extremely versatile and produces a light weight and reliable immobilizer.

Dynamics of cryogenic jets: non-rayleigh breakup and onset of nonaxisymmetric motions.

We report development of generators for periodic, satellite-free fluxes of monodisperse drops with diameters down to 10 microm from cryogenic liquids such as H2, N2, Ar, and Xe (and, as a reference fluid, water). While the break up of water jets can be described well by Rayleigh's linear theory, we find jet regimes for H2 and N2 which reveal deviations from this behavior. Thus, Rayleigh's theory is inappropriate for thin jets that exchange energy and/or mass with the surrounding medium. Moreover, at high evaporation rates, the axial symmetry of the dynamics is lost. When the drops pass into vacuum, frozen pellets form due to surface evaporation. The narrow width of the pellet flux paves the way towards various industrial and scientific applications.

Precision study of the eta3He system using the dp--> 3Heeta reaction.

The differential and total cross sections for the dp--> 3Heeta reaction have been measured in a high precision high statistics COSY-ANKE experiment near threshold using a continuous beam energy ramp up to an excess energy Q of 11.3 MeV with essentially 100% acceptance. The kinematics allowed the mean value of Q to be determined to about 9 keV. Evidence is found for the effects of higher partial waves for Q >or= 4 MeV. The very rapid rise of the total cross section to its maximum value within 0.5 MeV of threshold implies a very large eta3He scattering length and hence the presence of a quasibound state extremely close to threshold.

Evidence for an excited hyperon state in pp --> pK+Y0*.

Indications for the production of a neutral excited hyperon in the reaction pp --> pK+Y0* are observed in an experiment performed with the ANKE spectrometer at COSY-Jülich at p(beam) = 3.65 GeV/c. Two final states were investigated simultaneously, viz. Y0* --> pi+X- and pi-X+, and consistent results were obtained in spite of the quite different experimental conditions. The parameters of the hyperon state are M(Y0*) = (1480 +/-15) MeV/c2 and gamma(Y0*) = (60 +/- 15) MeV/c2. The production cross section for Y0* decaying through these channels is of the order of few hundred nanobarns. Since the isospin of the Y0* has not been determined here, it could either be an observation of the sigma(1480), a one-star resonance of the Particle Data Group tables, or, alternatively, a lambda hyperon. Relativistic quark models for the baryon spectrum do not predict any excited hyperon in this mass range and so the Y0* may be of exotic nature.

Precision measurement of the quasifree pn-->dvarphi reaction close to threshold.

The quasifree pn-->dvarphi reaction has been studied at the Cooler Synchrotron COSY-Jülich, using the internal proton beam incident on a deuterium cluster-jet target and detecting a fast deuteron in coincidence with the K+K- decay of the varphi meson. The energy dependence of the total and differential cross sections are extracted for excess energies up to 80 MeV by determining the Fermi momentum of the target neutron on an event-by-event basis. Though these cross sections are consistent with s-wave production, the kaon angular distributions show the presence of p waves at quite a low energy. Production on the neutron is found to be stronger than on the proton but not by as much as for the eta meson.

Near-threshold production of phi mesons in pp collisions.

The pp-->ppphi reaction has been studied at the Cooler Synchrotron COSY-Jülich, using the internal beam and ANKE facility. Total cross sections have been determined at three excess energies epsilon near the production threshold. The differential cross section closest to threshold at epsilon=18.5 MeV exhibits a clear S wave dominance as well as a noticeable effect due to the proton-proton final-state interaction. Taken together with data for ppomega production, a significant enhancement of the phi/omega ratio of a factor 8 is found compared to predictions based on the Okubo-Zweig-Iizuka rule.