Published 1977
| Version v1
Report
Transition density of the octupole vibration in 208Pb. Comparison of theory and experiment
Description
The transition charge density for lead 208 was calculated using random phase approximation calculations and is shown. It has a large peak centered at the nuclear surface at abour r = 7fm and pronounced oscillations in the interior of the nucleus for 0 less than or equal to r less than or equal to 5 fm. With the hydrodynamic or the Tassie model the transition density can be related to the ground state charge density. It is noted that the fluctuations in the ground state charge density are not at all large enough to explain the observed oscillations. The structure of this transition strength is described. A comparison is given of experimental data for sigma/sigma/sub Mott/ to theoretical predictions for the 3- state in 208Pb. 14 references
Additional details
Additional titles
- Augmented title (English)
- Random phase approximation
Publishing Information
- Imprint Title
- Proceedings of the June workshop in intermediate energy electromagnetic interactions with nuclei, held at MIT, June 13-24, 1977
- Journal Page Range
- p. 355-362A.
- Report number
- COO--3069-677
INIS
- Country of Publication
- United States
- Country of Input or Organization
- United States
- INIS RN
- 11512468
- Subject category
- S73: NUCLEAR PHYSICS AND RADIATION PHYSICS;
- Resource subtype / Literary indicator
- Numerical Data
- Descriptors DEI
- CHARGE DENSITY; CROSS SECTIONS; ELECTRON REACTIONS; ENERGY LEVELS; ENERGY-LEVEL TRANSITIONS; GRAPHS; GROUND STATES; HYDRODYNAMIC MODEL; LEAD 208; MOTT SCATTERING; OSCILLATIONS; PARITY; SPIN; SURFACES; THEORETICAL DATA; VIBRATIONAL STATES
- Descriptors DEC
- ANGULAR MOMENTUM; DATA; DATA FORMS; ELASTIC SCATTERING; EVEN-EVEN NUCLEI; EXCITED STATES; HEAVY NUCLEI; INFORMATION; ISOTOPES; LEAD ISOTOPES; LEPTON REACTIONS; MATHEMATICAL MODELS; NUCLEAR REACTIONS; NUCLEI; NUMERICAL DATA; PARTICLE MODELS; PARTICLE PROPERTIES; SCATTERING; STABLE ISOTOPES; STATISTICAL MODELS; THERMODYNAMIC MODEL