Isoscalar breathing mode state in /sup 90/Zr and /sup 116/Sn
Beams of 96- and 129-MeV ..cap alpha.. particles were used to excite the giant resonance region in /sup 90/Zr and /sup 116/Sn. From the analysis of data obtained from 0/sup 0/ to 8/sup 0/, two distinct components of the giant resonance peak were resolved in each nucleus. The upper component is well described by a distorted-wave Born-approximation calculation for L=0 exhausting 90% (180%) of the energy weighted sum rule and has E/sub x/=16.2 MeV (15.6 MeV), GAMMA=3.5 MeV (4.1 MeV) for /sup 90/Zr (/sup 116/Sn). The nuclear incompressibility is extracted from these data and from that available for /sup 144/Sm and /sup 208/Pb. The lower component is the giant quadrupole resonance exhausting 66% (84%) of the isoscalar quadrupole sum rule and has E/sub x/=14.0 MeV (13.2 MeV), GAMMA=3.4 MeV (3.3 MeV) for /sup 90/Zr (/sup 116/Sn).
- Research Organization:
- Cyclotron Institute, Texas AM University, College Station, Texas 77843
- OSTI ID:
- 5409204
- Journal Information:
- Phys. Rev., C; (United States), Vol. 21:4
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
ALPHA REACTIONS
INELASTIC SCATTERING
TIN 116
GIANT RESONANCE
TIN 116 TARGET
ZIRCONIUM 90
ZIRCONIUM 90 TARGET
ALPHA SPECTRA
ANGULAR DISTRIBUTION
CROSS SECTIONS
DWBA
MEV RANGE 10-100
MEV RANGE 100-1000
NUCLEAR MATTER
PROPORTIONAL COUNTERS
QUADRUPOLE MOMENTS
SUM RULES
TIME-OF-FLIGHT METHOD
BORN APPROXIMATION
CHARGED-PARTICLE REACTIONS
DISTRIBUTION
ENERGY RANGE
EQUATIONS
EVEN-EVEN NUCLEI
INTERMEDIATE MASS NUCLEI
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
MATTER
MEASURING INSTRUMENTS
MEV RANGE
NUCLEAR REACTIONS
NUCLEI
RADIATION DETECTORS
RADIOISOTOPES
RESONANCE
SCATTERING
SPECTRA
STABLE ISOTOPES
TARGETS
TIN ISOTOPES
ZIRCONIUM ISOTOPES
651723* - Nuclear Properties & Reactions
A=90-149
Experimental- Energy Levels & Transitions- (-1987)
651725 - Nuclear Properties & Reactions
A=90-149
Experimental- Nuclear Reactions & Scattering- (-1987)