3s/sub 1/2/ spectroscopic strength distribution in /sup 207/Tl and /sup 205/Tl
Journal Article
·
· Phys. Rev. C; (United States)
The fragmentations of the five proton hole states, 3s/sub 1/2/, 2d/sub 3/2/, 1h/sub 11/2/, 2d/sub 5/2/, and 1g/sub 7/2/, in /sup 207/Tl and /sup 205/Tl are calculated in terms of the coupling of these states with the collective vibrational states in /sup 208/Pb and /sup 206/Pb, respectively. Good overall agreement is observed between the experimental and theoretical results. The calculated occupancy of the 3s/sub 1/2/ state in /sup 208/Pb is n(208) = 0.94, as compared to the (e,e'p) reaction result n(208) = 0.83(9) and the (d,/sup 3/He) reaction result n(208) = 0.92(13). Several weak (S/sub j/less than or equal to0.02) 3s/sub 1/2/ states are predicted in /sup 207/Tl and /sup 205/Tl.
- Research Organization:
- Saha Institute of Nuclear Physics, Calcutta 700 064, India
- OSTI ID:
- 5548942
- Journal Information:
- Phys. Rev. C; (United States), Journal Name: Phys. Rev. C; (United States) Vol. 36:6; ISSN PRVCA
- Country of Publication:
- United States
- Language:
- English
Similar Records
Relative 3s-italic spectroscopic strength in /sup 206/Pb and /sup 208/Pb studied with the (e-italic,e-italic/sup '/p) knockout reaction
Intermediate coupling in /sup 203/ /sup 205/Tl. [. gamma. angular distributions from /sup 203/ /sup 205/Tl(n, n. gamma. ) reactions]
Core polarization effect on the discrete proton hole states of [sup 205]Tl
Journal Article
·
Mon Jul 14 00:00:00 EDT 1986
· Phys. Rev. Lett.; (United States)
·
OSTI ID:5379848
Intermediate coupling in /sup 203/ /sup 205/Tl. [. gamma. angular distributions from /sup 203/ /sup 205/Tl(n, n. gamma. ) reactions]
Journal Article
·
Mon Jan 31 23:00:00 EST 1977
· Phys. Rev., C; (United States)
·
OSTI ID:7228605
Core polarization effect on the discrete proton hole states of [sup 205]Tl
Journal Article
·
Thu Dec 31 23:00:00 EST 1992
· Physical Review, C (Nuclear Physics); (United States)
·
OSTI ID:6831901
Related Subjects
653001* -- Nuclear Theory-- Nuclear Structure
Moments
Spin
& Models
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
BARYONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
CHARGE DENSITY
CHARGED-PARTICLE REACTIONS
DEUTERON REACTIONS
ELECTRON REACTIONS
ELEMENTARY PARTICLES
ENERGY LEVELS
EVEN-EVEN NUCLEI
EVEN-ODD NUCLEI
EXCITED STATES
FERMIONS
FRAGMENTATION
FUNCTIONS
HADRONS
HEAVY NUCLEI
HELIUM 3
HELIUM ISOTOPES
ISOTOPES
LEAD 206
LEAD 208
LEAD ISOTOPES
LEPTON REACTIONS
LIGHT NUCLEI
MATHEMATICAL MODELS
MINUTES LIVING RADIOISOTOPES
NUCLEAR MODELS
NUCLEAR POTENTIAL
NUCLEAR REACTIONS
NUCLEAR STRUCTURE
NUCLEI
NUCLEONS
ODD-EVEN NUCLEI
POTENTIALS
PROTONS
RADIOISOTOPES
SHELL MODELS
STABLE ISOTOPES
STRENGTH FUNCTIONS
THALLIUM 205
THALLIUM 207
THALLIUM ISOTOPES
VIBRATIONAL STATES
WOODS-SAXON POTENTIAL
Moments
Spin
& Models
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
BARYONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
CHARGE DENSITY
CHARGED-PARTICLE REACTIONS
DEUTERON REACTIONS
ELECTRON REACTIONS
ELEMENTARY PARTICLES
ENERGY LEVELS
EVEN-EVEN NUCLEI
EVEN-ODD NUCLEI
EXCITED STATES
FERMIONS
FRAGMENTATION
FUNCTIONS
HADRONS
HEAVY NUCLEI
HELIUM 3
HELIUM ISOTOPES
ISOTOPES
LEAD 206
LEAD 208
LEAD ISOTOPES
LEPTON REACTIONS
LIGHT NUCLEI
MATHEMATICAL MODELS
MINUTES LIVING RADIOISOTOPES
NUCLEAR MODELS
NUCLEAR POTENTIAL
NUCLEAR REACTIONS
NUCLEAR STRUCTURE
NUCLEI
NUCLEONS
ODD-EVEN NUCLEI
POTENTIALS
PROTONS
RADIOISOTOPES
SHELL MODELS
STABLE ISOTOPES
STRENGTH FUNCTIONS
THALLIUM 205
THALLIUM 207
THALLIUM ISOTOPES
VIBRATIONAL STATES
WOODS-SAXON POTENTIAL