The Experimental Astrophysics group at the Goethe University

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The Experimental Astrophysics group at the Goethe University Frankfurt http: //exp-astro. physik. uni-frankfurt. de/

The Experimental Astrophysics group at the Goethe University Frankfurt http: //exp-astro. physik. uni-frankfurt. de/ Currently: • 5 scientists • 12 Ph. D students • 8 students Experimental Astrophysics at the Goethe University Frankfurt

Activities • With strong ties to n-TOF – measurments of (n, g) cross sections

Activities • With strong ties to n-TOF – measurments of (n, g) cross sections (motivated by astrophysics but also applied) – Complementary measurements at FRANZ (cleaner background and higher fluxes in ke. V regime) and n-TOF (wide spectrum, superior neutron energy resolution) – (n, a), (n, p) cross sections in similar fashion – Development of high-performance DAQ (FPGA+FADC) – Development of neutron- / gamma detectors, tests (LENA, Neu. LAND) • General Portfolio: – Determination of reaction cross sections with astrophysical relevance (n-, p-, a-, g-induced) – Specialized in measurments on / with radioactive isotopes – p-induced: Experimental Astrophysics at the Goethe University Frankfurt

Neutron-induced reactions • FRANZ – TOF (10 cm, 1 m flightpath) – Activation –

Neutron-induced reactions • FRANZ – TOF (10 cm, 1 m flightpath) – Activation – (n, g), (n, a), (n, f) • n-TOF – TOF (10 m, 180 m flightpath) • DANCE / Los Alamos – TOF (20 m flightpath) Experimental Astrophysics at the Goethe University Frankfurt

Detector for Advanced Neutron Capture Experiments neutrons: • spallation source • thermal. . 500

Detector for Advanced Neutron Capture Experiments neutrons: • spallation source • thermal. . 500 ke. V • 20 m flight path • 3 105 n/s/cm 2/decade collimated neutrons beam g-Detector: sample t 1/2 > 100 d m ~ 1 mg 34 cm • 160 Ba. F 2 crystals • 4 different shapes • Ri=17 cm, Ra=32 cm • 7 cm 6 Li. H inside • eg 90 % • ecasc 98 % Experimental Astrophysics at the Goethe University » Nuclear. Frankfurt Astrophysics with Neutron Facilities and LANL and RIA «

The Frankfurt neutron source at the Stern-Gerlach. Zentrum (FRANZ) 20 m. A DC neutron

The Frankfurt neutron source at the Stern-Gerlach. Zentrum (FRANZ) 20 m. A DC neutron flux: 1012 s-1 2 m. A proton beam (8 A peak current) 250 k. Hz < 1 ns pulse width neutron flux at 1 m: 107 s-1 cm-2 neutron flux at 0. 1 m: 109 s-1 cm-2 Experimental Astrophysics at the Goethe University Frankfurt

Neutron spectrum Quasi-Maxwellian averaged distribution: k. T = Emax = Experimental Astrophysics at the

Neutron spectrum Quasi-Maxwellian averaged distribution: k. T = Emax = Experimental Astrophysics at the Goethe University Frankfurt 25 ke. V 110 ke. V

Effect of proton energy uncertainty • Ep = 1912 ke. V • different proton

Effect of proton energy uncertainty • Ep = 1912 ke. V • different proton energy distributions • 30 µm lithium • 10 mm diameter gold foils • weighting of sample thickness for different neutron angles considered Experimental Astrophysics at the Goethe University Frankfurt

Ep=2200 ke. V, 5 µmx 3 mm Li, 3 mm sample Experimental Astrophysics at

Ep=2200 ke. V, 5 µmx 3 mm Li, 3 mm sample Experimental Astrophysics at the Goethe University Frankfurt

Ep=2100 ke. V, 5 µmx 3 mm Li, 3 mm sample Experimental Astrophysics at

Ep=2100 ke. V, 5 µmx 3 mm Li, 3 mm sample Experimental Astrophysics at the Goethe University Frankfurt

Ep=1980 ke. V, 1 µmx 3 mm Li, 3 mm sample Experimental Astrophysics at

Ep=1980 ke. V, 1 µmx 3 mm Li, 3 mm sample Experimental Astrophysics at the Goethe University Frankfurt

The 4 p Ba. F 2 array for TOF measurements Hardware: • g-calorimeter –

The 4 p Ba. F 2 array for TOF measurements Hardware: • g-calorimeter – 15 cm thick – eg, total ~ 90 % – ecasc, total ~ 98 % – ecasc, peak ~ 50 % • • 96 channels 1 GS/s FADC + FPGA 30 TB RAID array Allows: • Particle identification • deadtime-less DAQ • pile-up correction • fast data reduction Experimental Astrophysics at the Goethe University Frankfurt

Schematic TOF spectrum 200 128 En (ke. V) • 80 cm flight path •

Schematic TOF spectrum 200 128 En (ke. V) • 80 cm flight path • 10 cm inner detector radius • Emax = 200 ke. V • Emin = 1 ke. V prompt flash other reactions (n, g) on sample 0 130 160 Experimental Astrophysics at the Goethe University Frankfurt TOF (ns)

The Frankfurt neutron source at the Stern-Gerlach. Zentrum (FRANZ) neutron flux: 1012 s-1 2

The Frankfurt neutron source at the Stern-Gerlach. Zentrum (FRANZ) neutron flux: 1012 s-1 2 m. A proton beam (8 A peak current) 250 k. Hz < 1 ns pulse width neutron flux at 1 m: 107 s-1 cm-2 neutron flux at 0. 1 m: 109 s-1 cm-2 sample TOF with 10 cm flightpath using fast charged particle detectors: Si-diode, C-diamond, ionization chamber Experimental Astrophysics at the Goethe University Frankfurt

Proton-induced reactions • (p, g), (p, n) – FRANZ (high currents, limited energy range)

Proton-induced reactions • (p, g), (p, n) – FRANZ (high currents, limited energy range) – Experimental storage ring (ESR) at GSI and maybe rex-isolde (goal: radioactive nuclei) • (p, n) – LAND/R 3 B setup, determination of Gamow. Teller strength, hence half-lifes under stellar conditions • (a, g) – Van de Graaff: Notre Dame – ESR (still to be shown) Experimental Astrophysics at the Goethe University Frankfurt

The Frankfurt neutron source at the Stern-Gerlach. Zentrum (FRANZ) 2 m. A proton beam

The Frankfurt neutron source at the Stern-Gerlach. Zentrum (FRANZ) 2 m. A proton beam (8 A peak current) 250 k. Hz Experimental Astrophysics at the Goethe University Frankfurt 20 m. A DC

Reaction Studies at the ESR Measurements of (p, g) or (α, g) rates in

Reaction Studies at the ESR Measurements of (p, g) or (α, g) rates in the Gamow window of the p-process in inverse kinematics. Particle detectors Advantages: • Applicable to radioactive nuclei • Detection of ions via in-ring particle detectors (low background, high efficiency) • Knowledge of line intensities of product nucleus not necessary • Applicable to gases Challenges: • UHV conditions • Low-energy beam • Detectors must be bakeable • Interaction with rest gas Experimental Astrophysics at the Goethe University Frankfurt Gas jet ESR

gamma-induced reactions • g-induced – Coulomb excitation (GSI) – direct (HIGS, ELBE) Experimental Astrophysics

gamma-induced reactions • g-induced – Coulomb excitation (GSI) – direct (HIGS, ELBE) Experimental Astrophysics at the Goethe University Frankfurt

Radioactive beam experiments for the s-process Idea: Determine AX(n, g) from nat. Pb(A+1 X,

Radioactive beam experiments for the s-process Idea: Determine AX(n, g) from nat. Pb(A+1 X, AX+n) Coulomb Dissociation of A+1 X gives A+1 X(g, n) Detailed balance gives AX(n, g) Experimental Astrophysics at the Goethe University Frankfurt

Detector developments for FAIR/GSI • Neutron detection between 0. 01 and 1 Me. V

Detector developments for FAIR/GSI • Neutron detection between 0. 01 and 1 Me. V – LENA • Neutron detection between 0. 1 and 1 Ge. V – Neu. LAND Experimental Astrophysics at the Goethe University Frankfurt

Neutron detection – 10 ke. V – 1 Me. V LENA ( low energy

Neutron detection – 10 ke. V – 1 Me. V LENA ( low energy neutron detector array): Detection of low energy neutrons with high angular resolution. Plastic scintillator bars 100 x 4. 5 x 1 cm Tests needed! time resolution energy threshold FWHM=0. 8 ns Experimental Astrophysics at the Goethe University Frankfurt

Neutron detection – 100 Me. V – 1 Ge. V Neu. LAND (New Large

Neutron detection – 100 Me. V – 1 Ge. V Neu. LAND (New Large Acceptance Neutron Detector): Detection of relativistic neutrons with high efficiency -60 layers of scintillator -each -5 cm deep , 2. 5 x 2. 5 m 2 cross section -Cosists of scintillator 40 bars (5 x 5 x 250 cm 3) Experimental Astrophysics at the Goethe University Frankfurt