46 research outputs found

    Gamma-widths, lifetimes and fluctuations in the nuclear quasi-continuum

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    Statistical γ\gamma-decay from highly excited states is determined by the nuclear level density (NLD) and the γ\gamma-ray strength function (γ\gammaSF). These average quantities have been measured for several nuclei using the Oslo method. For the first time, we exploit the NLD and γ\gammaSF to evaluate the γ\gamma-width in the energy region below the neutron binding energy, often called the quasi-continuum region. The lifetimes of states in the quasi-continuum are important benchmarks for a theoretical description of nuclear structure and dynamics at high temperature. The lifetimes may also have impact on reaction rates for the rapid neutron-capture process, now demonstrated to take place in neutron star mergers.Comment: CGS16, Shanghai 2017, Proceedings, 5 pages, 3 figure

    Level densities and γ\gamma-strength functions in 148,149^{148,149}Sm

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    The level densities and γ\gamma-strength functions of the weakly deformed 148^{148}Sm and 149^{149}Sm nuclei have been extracted. The temperature versus excitation energy curve, derived within the framework of the micro canonical ensemble, shows structures, which we associate with the break up of Cooper pairs. The nuclear heat capacity is deduced within the framework of both the micro canonical and the canonical ensemble. We observe negative heat capacity in the micro canonical ensemble whereas the canonical heat capacity exhibits an S-shape as function of temperature, both signals of a phase transition. The structures in the γ\gamma-strength functions are discussed in terms of the pygmy resonance and the scissors mode built on exited states. The samarium results are compared with data for the well deformed 161,162^{161,162}Dy, 166,167^{166,167}Er and 171,172^{171,172}Yb isotopes and with data from (n,γ\gamma)-experiments and giant dipole resonance studies.Comment: 12 figure

    Statistical properties of the well deformed 153,155^{153,155}Sm nuclei and the scissors resonance

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    The Nuclear Level Densities (NLDs) and the γ\gamma-ray Strength Functions (γ\gammaSFs) of 153,155^{153,155}Sm have been extracted from (d,pγ\gamma) coincidences using the Oslo method. The experimental NLD of 153^{153}Sm is higher than the NLD of 155^{155}Sm, in accordance with microscopic calculations. The γ\gammaSFs of 153,155^{153,155}Sm are in fair agreement with QRPA calculations based on the D1M Gogny interaction. An enhancement is observed in the γ\gammaSF for both 153,155^{153,155}Sm nuclei around 3 MeV in excitation energy and is attributed to the M1 Scissors Resonance (SR). Their integrated strengths were found to be in the range 1.3 - 2.1 and 4.4 - 6.4 μN2\mu^{2}_{N} for 153^{153}Sm and 155^{155}Sm, respectively. The strength of the SR for 155^{155}Sm is comparable to those for deformed even-even Sm isotopes from nuclear resonance fluorescence measurements, while that of 153^{153}Sm is lower than expected

    New experimental constraint on the 185^{185}W(n,γn,\gamma)186^{186}W cross section

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    In this work, we present new data on the 182,183,184^{182,183,184}W(γ,n\gamma,n) cross sections, utilizing a quasi-monochromatic photon beam produced at the NewSUBARU synchrotron radiation facility. Further, we have extracted the nuclear level density and γ\gamma-ray strength function of 186^{186}W from data on the 186^{186}W(α,αγ\alpha,\alpha^\prime\gamma)186^{186}W reaction measured at the Oslo Cyclotron Laboratory. Combining previous measurements on the 186^{186}W(γ,n\gamma,n) cross section with our new 182,183,184^{182,183,184}W(γ,n\gamma,n) and (α,αγ\alpha,\alpha^\prime\gamma)186^{186}W data sets, we have deduced the 186^{186}W γ\gamma-ray strength function in the range of 1<Eγ<61 < E_\gamma < 6 MeV and 7<Eγ<147 < E_\gamma < 14 MeV. Our data are used to extract the level density and γ\gamma-ray strength functions needed as input to the nuclear-reaction code \textsf{TALYS}, providing an indirect, experimental constraint for the 185^{185}W(n,γn,\gamma)186^{186}W cross section and reaction rate. Compared to the recommended Maxwellian-averaged cross section (MACS) in the KADoNiS-1.0 data base, our results are on average lower for the relevant energy range kBT[5,100]k_B T \in [5,100] keV, and we provide a smaller uncertainty for the MACS. The theoretical values of Bao \textit{et al.} and the cross section experimentally constrained on photoneutron data of Sonnabend \textit{et al.} are significantly higher than our result. The lower value by Mohr \textit{et al.} is in very good agreement with our deduced MACS. Our new results could have implications for the ss-process and in particular the predicted ss-process production of 186,187^{186,187}Os nuclei.Comment: 17 pages, 15 figures; to be submitted to Phys. Rev.

    Nuclear Level Density and γ\gamma-ray Strength Function of 67Ni^{67}\mathrm{Ni} and the impact on the i-process

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    Proton-γ\gamma coincidences from (d,p)(\mathrm{d},\mathrm{p}) reactions between a 66Ni^{66}\mathrm{Ni} beam and a deuterated polyethylene target have been analyzed with the inverse Oslo method to find the nuclear level density (NLD) and γ\gamma-ray strength function (γ\gammaSF) of 67Ni^{67}\mathrm{Ni}. The 66Ni(n,γ)^{66}\mathrm{Ni}(\mathrm{n},\gamma) capture cross section has been calculated using the Hauser-Feshbach model in TALYS using the measured NLD and γ\gammaSF as constraints. We confirm that 66Ni(n,γ)^{66}\mathrm{Ni}(\mathrm{n},\gamma) acts as a bottleneck when relying on one-zone nucleosynthesis calculations. However, we find that the impact of this reaction is strongly damped in multi-zone low-metallicity AGB stellar models experiencing i-process nucleosynthesis.Comment: Submitted to Phys. Rev.

    Evolution of the γ\gamma-ray strength function in neodymium isotopes

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    The experimental gamma-ray strength functions (gamma-SFs) of 142,144-151Nd have been studied for gamma-ray energies up to the neutron separation energy. The results represent a unique set of gamma-SFs for an isotopic chain with increasing nuclear deformation. The data reveal how the low-energy enhancement, the scissors mode and the pygmy dipole resonance evolve with nuclear deformation and mass number. The data indicate that the mechanisms behind the low-energy enhancement and the scissors mode are decoupled from each other.Comment: 14 pages and 10 figure
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