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NNSA Synergistic Activities at TUNL The Triangle Universities Nuclear Lab is developing excellent facilities for studying (n, xn ) reactions. Resources provided through NNSA/DOE grant #DE-PS52-05NA25930 have supplied four HPGE Clover Detectors, two Planar Detectors and supporting equipment. The research program at TUNL has developed components that utilize these resources to support both SSAA mission objectives and other curiosity driven nuclear-physics research objectives. HPGe and Planar -ray detectors are supported on moveable plates that can cover lab angles ranging from 20 O to 160 O . A liquid scintillator neutron detector is positioned 2.0-meters from the target (at 0 O ) to monitor the neutron beam characteristics and flux. A second neutron beam area in the “NTOF Target Room” comprises a nominally unshielded neutron production cell that has been used in our 241 Am(n, 2n) activation measurements. We plan to add a third neutron beam-line that is dedicated to this work. Neutron Beam Facility & -ray Detectors Insight into relevance of neutron induced reactions in deep underground experiments Activities Supported in part by the NNSA under the Stewardship Science Academic Alliances Program DOE grant #DE-PS52-05NA25930, and by DOE DE-FG02-97ER41033 (Duke) and DE-FG02-97ER41042 (NC-State). I d =1A 7.8 atm beam pickoff 2 H(d,n) 3 He COPPER For the past several years, the TUNL REU program has started their 10-week summer session by measuring 28 Si, 32 S(n, n’ ) scattering using the NNSA HPGe array and TUNL’s NaI and liquid- scintillator detectors. This two-day exercise, which includes detector and electronics set-up, data taking and analysis, and oral presentation of observations introduces students to basic laboratory techniques and demonstrates the utility of high resolution spectroscopy for materials identification. The Majorana Experiment Expected 0 Signal 2039 keV peak 2039 keV REU Student REU Student Projects Projects Open questions that can be addressed in 2 decay studies : Are Majorana particles? (self anti- particles) Is lepton number conserved? (Standard Model) observation yields neutrino mass could give insight into neutrino mass Backgrounds from Pb(n,2n ) Cu(n,2n ) Time Reaction Energies[MeV] May 2003 238 U(n,2nγ) 237 U En = 6, 10 Aug 2004 238 U(n,2n γ) 237 U En = 8, 10, 14 Feb 2005 90 Zr(n,n'γ) 90 Zr En = 6 Feb 2005 89 Yb(n,n'γ) 89 Yb En = 6 Feb 2005 112 Sn(n,n'γ) 112 Sn En = 6.5, 7.5, 8.0 Feb 2005 124 Sn(n,n'γ) 124 Sn En = 6.5, 7.5, 8.0 May 2005 235 U(n,n'γ) 235 U En = 5 Jun 2005 235 U(n,2n'γ) 234 U En = 12 Jun 2005 nat Hf(n,xn'γ) En = 12 Jun 2005 16 O(n,n'γ) 16 O En = 7 Jun 2005 12 C(n,n'γ) 12 C En = 7 Dec 2005 235 U(n,2n'γ) 234 U En = 12.0 Jan 2006 235 U(n,2n'γ) 234 U En = 10.0, 8.0 Jan 2006 181 Ta(n,2n'γ) 180 Ta En = 14.5 Feb 2006 140 Ce(n,2n'γ) 139 Ce En = 14.5 2006 94 Zr(n,n’) 94 Zr En = 5 2006 241 Am(n,2n) Activation En 8-14 Jun 2006 nat Cu, nat Pb(n,n’) En=8,12 Oct 2006 235,238 U(n, 2n) En=10 Dec 2006 241 Am(n,2n) Activation En=8-16 Dec 2006 235 U(n, 2n) 253 U En=12 Jan 2007 235 U(n,2n) 235 U En=8 Since 2003 a variety of measurements have been carried out utilizing the TUNL neutron beam-lines and the NNSA funded HPGe detector array. Our efforts are dominated by studies in the actinide region, though additional measurements have contributed interests in other projects, and student training exercises. Two experimental halls at TUNL are dedicated to neutron beam research. In the Shielded Neutron Source Area (above) neutrons can be produced using either the 2 H(d,n) or 3 H(p,n) reaction. The ion beams are chopped and bunched prior to entering the FN Tandem accelerator. A copper collimator defines the neutron beam size and trajectory; further beam cleanup is provided by Pb and Li- doped plastic shielding. In early 2006 we collaborated with Steve Yates et al., from the University of Kentucky to carry out a study of mixed symmetry states in 94 Zr. In this experiment we utilized the high efficiency of our clover array, by measuring 94 Zr(n,n’ ) two -ray coincidence data. Preliminary results were presented at the DNP meeting in Nashville. J.H. Kelley 1 , B. Fallin 2 , A. Hutcheson 2 , H.J. Karwowski 3 , E. Kwan 2 , A.P. Tonchev 2 , W. Tornow 2 & Collaborators 1 Triangle Universities Nuclear Lab & North Carolina State University 2 Triangle Universities Nuclear Lab & Duke University 1 Triangle Universities Nuclear Lab & University of North Carolina at Chapel Hill

NNSA Synergistic Activities at TUNL The Triangle Universities Nuclear Lab is developing excellent facilities for studying (n, xn ) reactions. Resources

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Page 1: NNSA Synergistic Activities at TUNL The Triangle Universities Nuclear Lab is developing excellent facilities for studying (n, xn  ) reactions. Resources

NNSA Synergistic Activities at TUNL

The Triangle Universities Nuclear Lab is developing excellent facilities for studying (n, xn ) reactions. Resources provided through NNSA/DOE grant #DE-PS52-05NA25930 have supplied four HPGE Clover Detectors, two Planar Detectors and supporting equipment. The research program at TUNL has

developed components that utilize these resources to support both SSAA mission objectives and other curiosity driven nuclear-physics research objectives.

HPGe and Planar -ray detectors are supported on moveable plates that can cover lab angles ranging from 20O to 160O. A liquid scintillator neutron detector is positioned 2.0-meters from the target (at 0O) to monitor the neutron beam characteristics and flux. A second neutron beam area in the “NTOF Target Room” comprises a nominally unshielded neutron production cell that has been used in our 241Am(n, 2n) activation measurements. We plan to add a third neutron beam-line that is dedicated to this work.

Neutron Beam Facility & -ray Detectors

Insight into relevance of neutron induced reactions in deep underground experiments

Activities

Supported in part by the NNSA under the Stewardship Science Academic Alliances Program DOE grant #DE-PS52-05NA25930, and by

DOE DE-FG02-97ER41033 (Duke) and DE-FG02-97ER41042 (NC-State).

Id =1A

7.8 atmbeam

pickoff

2H(d,n)3He

COPPER

For the past several years, the TUNL REU program has started their 10-week summer session by measuring 28Si, 32S(n, n’ ) scattering using the NNSA HPGe array and TUNL’s NaI and liquid-scintillator detectors. This two-day exercise, which includes detector and electronics set-up, data taking and analysis, and oral presentation of observations introduces students to basic laboratory techniques and demonstrates the utility of high resolution spectroscopy for materials identification.

The Majorana Experiment

Expected 0 Signal 2039 keV peak

2039 keV

REU Student ProjectsREU Student Projects

Open questions that can be addressed in 2 decay studies :Are Majorana particles? (self anti-particles)Is lepton number conserved? (Standard Model)

observation yields neutrino mass

could give insight into neutrino mass hierarchy

Backgrounds from Pb(n,2n )Cu(n,2n )

Time Reaction Energies[MeV] May 2003 238U(n,2nγ)237U En = 6, 10 Aug 2004 238U(n,2n γ)237U En = 8, 10, 14Feb 2005 90Zr(n,n'γ)90Zr En = 6 Feb 2005 89Yb(n,n'γ)89Yb En = 6 Feb 2005 112Sn(n,n'γ)112Sn En = 6.5, 7.5, 8.0Feb 2005 124Sn(n,n'γ)124Sn En = 6.5, 7.5, 8.0 May 2005 235U(n,n'γ)235U En = 5 Jun 2005 235U(n,2n'γ)234U En = 12 Jun 2005 natHf(n,xn'γ) En = 12Jun 2005 16O(n,n'γ)16O En = 7 Jun 2005 12C(n,n'γ)12C En = 7 Dec 2005 235U(n,2n'γ)234U En = 12.0 Jan 2006 235U(n,2n'γ)234U En = 10.0, 8.0 Jan 2006 181Ta(n,2n'γ)180Ta En = 14.5 Feb 2006 140Ce(n,2n'γ)139Ce En = 14.52006 94Zr(n,n’)94Zr En = 5 2006 241Am(n,2n) Activation En 8-14Jun 2006 natCu, natPb(n,n’) En=8,12Oct 2006 235,238U(n, 2n) En=10Dec 2006 241Am(n,2n) Activation En=8-16Dec 2006 235U(n, 2n)253U En=12 Jan 2007 235U(n,2n)235U En=8

Since 2003 a variety of measurements have been carried out utilizing the TUNL neutron beam-lines and the NNSA funded HPGe detector array. Our efforts are dominated by studies in the actinide region, though additional measurements have contributed interests in other projects, and student training exercises.

Two experimental halls at TUNL are dedicated to neutron beam research. In the Shielded Neutron Source Area (above) neutrons can be produced using either the 2H(d,n) or 3H(p,n) reaction. The ion beams are chopped and bunched prior to entering the FN Tandem accelerator. A copper collimator defines the neutron beam size and trajectory; further beam cleanup is provided by Pb and Li-doped plastic shielding.

In early 2006 we collaborated with Steve Yates et al., from the University of Kentucky to carry out a study of mixed symmetry states in 94Zr. In this experiment we utilized the high efficiency of our clover array, by measuring 94Zr(n,n’ ) two -ray coincidence data. Preliminary results were presented at the DNP meeting in Nashville.

J.H. Kelley1, B. Fallin2, A. Hutcheson2, H.J. Karwowski3, E. Kwan2, A.P. Tonchev2, W. Tornow2 & Collaborators1Triangle Universities Nuclear Lab & North Carolina State University

2Triangle Universities Nuclear Lab & Duke University 1Triangle Universities Nuclear Lab & University of North Carolina at Chapel Hill