Structure of the 10Li nucleus investigated via the 9Li(d,p)10Li reaction
Creators
- Santi, P.1, 2, 3, 4, 5
- Kolata, J.J.1, 2, 3, 4, 5
- Guimaraes, V.1, 2, 3, 4, 5
- Peterson, D.1, 2, 3, 4, 5
- White-Stevens, R.1, 2, 3, 4, 5
- Rischette, E.1, 2, 3, 4, 5
- Bazin, D.1, 2, 3, 4, 5
- Sherrill, B.M.1, 2, 3, 4, 5
- Navin, A.1, 2, 3, 4, 5
- DeYoung, P.A.1, 2, 3, 4, 5
- Jolivette, P.L.1, 2, 3, 4, 5
- Peaslee, G.F.1, 2, 3, 4, 5
- Guray, R.T.1, 2, 3, 4, 5
- 1. Physics Department, Ohio State University, Columbus, Ohio 43210 (United States)
- 2. Chemistry Department, Hope College, Holland, Michigan 49422-9000 (United States)
- 3. Physics Department, Hope College, Holland, Michigan 49422-9000 (United States)
- 4. National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824-1321 (United States)
- 5. Physics Department, University of Notre Dame, Notre Dame, Indiana 46556-5670 (United States)
Description
The structure of the particle unbound nucleus 10Li was investigated in a kinematically complete experiment using the 9Li(d,p)10Li reaction in inverse kinematics at an incident 9Li energy of 20 MeV/nucleon. The experiment utilized the S800 Spectrograph at the National Superconducting Cyclotron Laboratory to measure the outgoing 9Li from the breakup of 10Li in coincidence with the recoiling protons from the (d,p) reaction which were measured using an array of silicon detectors. Based on the kinematics of the recoiling protons from the 9Li(d,p) reaction, we measured a lower limit of Δ=33.10±0.08 MeV (i.e., Δ>33.02 MeV) for the mass excess of 10Li which is consistent with previous measurements. Through the complete reconstruction of the breakup kinematics, the structure of 10Li associated with a ground state 9Li core was distinguishable from structure associated with a 9Li core in its first excited state. The observed ratio of 9Li* core events to the total number of 10Li events that were detected in the experiment was 0.10±0.04 at forward center of mass angles (2.7 deg. to 9.5 deg.), and 0.24±0.03 at more backward center of mass angles (11 deg. to 26 deg.). The resulting Q-value spectra was best fit with either a single resonance located at Q=-2.58(11) MeV [corresponding to a neutron separation energy Sn=-0.35(11) MeV] or two resonances located at Q=-3.00(24) MeV [Sn=-0.77(24) MeV] and Q>-2.43 MeV (Sn>-0.2 MeV)
Additional details
Identifiers
Publishing Information
- Journal Title
- Physical Review. C, Nuclear Physics
- Journal Volume
- 67
- Journal Issue
- 2
- Journal Page Range
- p. 024606-024606.12
- ISSN
- 0556-2813
- CODEN
- PRVCAN
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 36012429
- Subject category
- S73: NUCLEAR PHYSICS AND RADIATION PHYSICS;
- Descriptors DEI
- DEUTERON REACTIONS; EXCITED STATES; GROUND STATES; LITHIUM 10; LITHIUM 9 TARGET; MEV RANGE; NEUTRON SEPARATION ENERGY; NUCLEAR STRUCTURE; PROTONS; Q-VALUE; RECOILS; RESONANCE; SI SEMICONDUCTOR DETECTORS; SUPERCONDUCTING CYCLOTRONS
- Descriptors DEC
- ACCELERATORS; BARYONS; BINDING ENERGY; CHARGED-PARTICLE REACTIONS; CYCLIC ACCELERATORS; CYCLOTRONS; ELEMENTARY PARTICLES; ENERGY; ENERGY LEVELS; ENERGY RANGE; FERMIONS; HADRONS; ISOTOPES; LIGHT NUCLEI; LITHIUM ISOTOPES; MEASURING INSTRUMENTS; MILLISECONDS LIVING RADIOISOTOPES; NUCLEAR REACTIONS; NUCLEI; NUCLEONS; ODD-ODD NUCLEI; RADIATION DETECTORS; RADIOISOTOPES; SEMICONDUCTOR DETECTORS; TARGETS
Optional Information
- Notes
- (c) 2003 The American Physical Society