Difference between revisions of "Forest NucPhys I Nuclear Reactions"
Jump to navigation
Jump to search
Line 47: | Line 47: | ||
This is typically a low energy reaction in which particle Y doesn't leave the target material but the intermediate state may be surmised at through the detection of particle b. | This is typically a low energy reaction in which particle Y doesn't leave the target material but the intermediate state may be surmised at through the detection of particle b. | ||
− | [[Image:CompoundReaction_Forest_Nucl_I.png | 500 px]] | + | [[Image:CompoundReaction_Forest_Nucl_I.png | 500 px]][[Image:CompoundReaction_nf_Forest_Nucl_I.png | 500 px]] |
− | |||
=Isospin= | =Isospin= |
Revision as of 22:52, 8 April 2009
Nuclear Reactions
Types of Reactions
- elastic scattering
- X & Y and a & b are the same particles, momentum and energy are conserved, typically all are in their ground state
- In-elastic scattering
- If Y or b are in an excited state, energy is not conserved it is used to excite one of the exiting particles.
- Note
- Elastic collisions are usually referred to as collisions and not nuclear reactions.
Direct Reactions
- knockout reaction
- a & b are the same but there are 3 total particles in the final state.
- n + X \rightarrow Y + 3n = X(n,3n)Y
- Transfer Reaction
- a nuclear from projectile a is transfered to target X
- Nuclear PhotoEffect
- projectile a ejects a nucleon from target X
- e - + Mo-100 \rightarrow Mo-99 + n + e- = X(e,e'n)Y
Capture
Compound reactions
- Compound reaction
- projectiel a is captured by target X forming an intermediate state which then decays, possibly through multiple excited nuclear states/species, to Y and b
This is typically a low energy reaction in which particle Y doesn't leave the target material but the intermediate state may be surmised at through the detection of particle b.
Isospin
14 nucleon system
Consider three different nuclear isobars all containing 14 nucleons ( isotopes are same Z, isotones are same N, so isobars are same A)
, ,
Experimentally it is observed that
has a half life of about 5000 years and a .
When it does decay it goes to
by emitting a \beta^- particle with a Q value of 156.473 keV.The
state it goes to hashttp://ie.lbl.gov/toi/nuclide.asp?iZA=60014
is stable.
The ground state of
has a half life of about 70.61 seconds and a .When it does decay it goes to
by emitting a \beta^+ particle with a Q value of 5.143 MeV.