A moving microfoil conversion electron detector for selective excitation double Mössbauer experiments

A lightweight microfoil conversion electron detector has been built for use as a detector/analyser for selective excitation double Mössbauer experiments. The detector weighs approximately 40 g; it can be moved with constant acceleration by a conventional electromechanical drive, with peak velocities up to ±15 mm/s. Conversion electrons from resonant absorption events are collected from both sides of two 0.3 μm thick⁵⁷Fe-enriched stainless steel foils inside the detector. The detector's performance (signal to noise per unit time) has been compared with a potassium ferrocyanide absorber and proportional counter, and it is found to be about ten times better for a given source strength and sampling angle. The overall detector linewidth is 0.42 (2) mm/s, compared with 0.37 (1) mm/s for the PFC absorber.     

Experimental beta-decay energies of short-lived light fission products

The beta-decay energy of 20 nuclides in the mass region 88≦A≦102 has been measured using the on-line mass separator LOHENGRIN. The experimental values obtained are compared with theoretical predictions of different mass formulae.     

Gamma-ray spectroscopy of short-lived fission products using the recoil separator “Lohengrin”

γ-spectra and half-lives of⁹⁰Br,⁹⁵Rb,⁹⁶Rb,⁹⁶Sr,⁹⁶Y,¹³²Sb and¹³²Sn have been measured using the unslowed fission fragment separator “Lohengrin”. Preliminary decay schemes for⁹⁰Kr,⁹⁵Sr,⁹⁶Sr and⁹⁶Y are given.     

Charge distributions in low-energy nuclear fission and their relevance to fission dynamics

Radiochemical and energy loss techniques have been used to measure fragment charge distributions in the systems ²²⁹Th(n_th, f), ²³⁵U(n_{3 MeV}, f) and ²⁵²Cf(s, f). Together with those previously obtained [^{233, 235}U(n_th, f) and ^{239, 241}Pu(n_th, f] the results show that these charge distributions depend very sensitively on both the fissioning species and the initial excitation energy. Very strong even-odd effects are present, for example in the charge distribution of ²²⁹Th(n_th, f) while they almost disappear in ²³⁵U(n_{3 MeV}, f). In the ²²⁹Th(n_th f) and ²⁵²Cf(s, f) cases, kinetic energy distributions of the fragments have been obtained. Fragments with even charges are more energetic, on average, than fragments with odd charges. The results are discussed in terms of a rather small probability for pair breaking during the transition from saddle-point to scission. The relationship between even-odd effects in charge distributions and fine structures in mass distributions is also investigated.     

Measurement of charge distributions for 229Th(nth,f) and 232U(nth,f)

A gas ΔE ? E_R telescope has been used to measure charge yields and their correlations with kinetic energies for ²²⁹Th and ²³²U. Even-charge yields are enhanced compared with odd-charge yields for both fissioning systems; this enhancement increases for events with higher kinetic energy. The mean odd-even effect $\text{δ}{}_{\mathrm{<mtext>p</mtext>}}\text{is}\text{= (40±4)\%}\text{for}{}^{229}\text{Th}$; it is $\text{(21 ± 3)\%}\text{for}{}^{232}\text{U-the same as for}{}^{233}\text{U}\text{((22.1±2.1)\%)}\text{and}{}^{235}\text{U}\text{((23.7±0.7)\%)}$. The energy-integrated δ_p and δ_p for different energy windows, vary strongly as a function of charge (Z) due to the underlying shells. The δ_p averaged over Z increases fast with kinetic energy, contrary to the existing results for ²³³U and ²³⁵U, where δ_p flattens off at low energies. For both systems, the most probable kinetic energy ē shows a strong odd-even stagger; the mean odd-even effect on energy, $\text{δE}{}_{\mathrm{<mtext>K</mtext>}}{}^{\mathrm{<mtext>o?e</mtext>}}\text{,}\text{is}\text{1.4 ± 0.3}\text{MeV for}{}^{229}\text{Th, and}\text{1.7±0.4}\text{MeV for}{}^{232}\text{U}\text{—}$ the latter is about twice the value for ${}^{233}\text{U}\text{(0.95 ± 0.09}\text{MeV}\text{)}\text{and}{}^{235}\text{U}\text{(0.7}\text{MeV}\text{)}$. These results are discussed in terms of the existing models.     

Étude de la phényl-2 oxine et de ses chélates: Constantes de dissociation de la phényl-2 oxine

The authors determined, by spcctrophotometric and potentiometric methods, the ionization constants of 2-phenyl-8-quinolinol in hydroalcoholic solutions.     

The first self-assembled trimetallic lanthanide helicate: different coordination sites in symmetrical molecular architectures

A tris-tridentate segmental ligand has been designed for the self-assembly of homotrimetallic triple-stranded lanthanide helicates possessing different coordination sites along the threefold axis.     

Polarization observable measurements for γp → K+Λ and γp → K+Σfor energies up to 1.5 GeV

Beam asymmetries and hyperon recoil polarizations for the reactions γp → K ⁺Λ and γp → K ⁺Σ⁰ have been measured from the threshold production to 1500MeV with the GRAAL facility located at the ESRF in Grenoble. These results complement the database for the beam asymmetry, covering for the first time the production threshold region. Recent theoretical analyses are presented for which the beam asymmetry data bring interesting new information and allow to better determine some resonance parameters. Most importantly, these results strengthen the need of a new D₁₃ state around 1900MeV.