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Neutron-induced Reactions

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Presentation on theme: "Neutron-induced Reactions"— Presentation transcript:

1 Neutron-induced Reactions
X(n,b)Y b(Q+En) n(En) Probability to penetrate the potential barrier Po(Ethermal) = 1 P>o(Ethermal) = 0 For thermal neutrons Q >> En b(Q)  constant Non-resonant Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

2 Neutron-induced Reactions
Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

3 Nuclear and Radiation Physics, BAU, 1st Semester, 2006-2007 (Saed Dababneh).

4 Neutron-induced Reactions
n-TOF CERN Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

5 Nuclear and Radiation Physics, BAU, 1st Semester, 2006-2007 (Saed Dababneh).

6 Neutron-induced Reactions
n_TOF CERN Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

7 Neutron-induced Reactions
Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

8 Charged Particle Reactions
What is the Gamow Peak? Nuclear Radius Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

9 Charged Particle Reactions
Electron Screening Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

10 Charged Particle Reactions
e2 = 1.44x10-12 keV.m Tunneling probability: In numerical units: For -ray emission: Sommerfeld parameter Gamow factor Multipolarity Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

11 Charged Particle Reactions
Nuclear (or astrophysical) S-factor Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

12 Charged Particle Reactions
EC = ?? Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

13 Resonance Reactions E  t
CN  particle emission  E  E > spacing between virtual states  continuum. (Lower part  larger spacing  isolated resonances). D  bound states  -emission  E  isolated states. Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

14 Resonance Reactions a + X  Y + b Q > 0 b + Y  X + a Q < 0
J Ex a + X  Y + b Q > 0 b + Y  X + a Q < 0 Excited State Entrance Channel a + X Exit Channel b + Y Inverse Reaction Compound Nucleus C* Identical particles Nature of force(s). Time-reversal invariance. Statistical Factor () QM HW 30 Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

15 (selected energies with large X-section)
Resonance Reactions Projectile Projectile Target Target Q-value Q-value Q + ER = Er E = E + Q - Eex Direct Capture (all energies) Resonant Capture (selected energies with large X-section) Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

16 Nuclear and Radiation Physics, BAU, 1st Semester, 2006-2007 (Saed Dababneh).

17 Resonance Reactions  HW 31
Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

18 Resonance Reactions Damped Oscillator Oscillator strength Damping
factor eigenfrequency Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

19 Resonance Reactions Breit-Wigner formula All quantities in CM system
Only for isolated resonances. Reaction Elastic scattering Usually a >> b. HW 32 When does R take its maximum value? Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

20 Resonance Reactions Ja + JX + l = J (-1)l (Ja) (JX) = (J)
Exit Channel b + Y Ja + JX + l = J (-1)l (Ja) (JX) = (J) (-1)l = (J) Natural parity. J Ex Excited State Entrance Channel a + X Compound Nucleus C* Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

21 radiative capture (a,)
Resonance Reactions What is the “Resonance Strength” …? What is its significance? In what units is it measured? Charged particle radiative capture (a,) (What about neutrons?) Cross section EC   a    Energy Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

22 Resonance Reactions 14N(p,) HW 33 Huge challenge to experimentalists
Q = ?? EC = ?? ER = 2.0 MeV Formation via s-wave protons, J = ½, p = 0.1 MeV, dipole radiation E = 9.3 MeV,  = 1 eV. Show that  = 0.33 eV. If same resonance but at ER = 10 keV p = ?? E = ??  = ?? Show that  = 3.3x10-23 eV. Huge challenge to experimentalists Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).

23 Resonance J Estimated
-transfer reactions Angular distribution Resonance J Estimated Energy (keV)  (eV) Experimental upper limit < 1.7 eV 18O(, )22Ne Nuclear and Radiation Physics, BAU, 1st Semester, (Saed Dababneh).


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