nuclear-reactions

Layer 1 — Physics24 concepts in this subtree

Kinematics, cross-sections, and resonance structure of reactions among atomic nuclei — the bridge from nuclear structure to astrophysical nucleosynthesis and applied nuclear engineering. Core conservation laws: baryon number A, charge Z,…

Q-value from mass defect: Q = (Σm_i − Σm_f)·c²
Breit-Wigner 1936 resonance: σ(E) Lorentzian with FWHM Γ
Gamow 1928 Coulomb-barrier tunnelling → stellar-fusion peak
²²⁶Ra → ²²²Rn + α Q-value: 5.230·10⁻³ u·c² exact (sym. rational)
Breit-Wigner FWHM = Γ exact (half-maximum solves to ±Γ/2)
Gamow peak E_0 = (E_G·(k_BT)²/4)^{1/3} exact saddle point
Gamow-peak saddle-point: maximum of f(E) = -E/kT - b/sqrt(E) at E_0 = (b kT / 2)^(2/3) * 2^(1/3)
Breit-Wigner Lorentzian sum rule: int_{-inf}^{inf} (gamma/2)^2 / ((E-E_R)^2 + (gamma/2)^2) dE = pi gamma / 2
Bethe level-density back-shifted Fermi-gas model: S(E) = 2 sqrt(aE); nuclear temperature T = sqrt(E/a)
Theorem: Gamow-peak saddle E_0 = 2^(1/3) b^(2/3) (k_BT)^(2/3) / 2 (unique positive real root)
Theorem: Lorentzian sum-rule integral = pi * gamma / 2 (residue theorem, contour in upper half-plane)
Theorem: Bethe Fermi-gas nuclear temperature T = sqrt(E)/sqrt(a) (thermodynamic 1/T = dS/dE)
Compound nucleus (Bohr 1936)
Optical model (1949)
Fission (Bohr-Wheeler 1939)
r-process (B2FH 1957)
RIB facilities
Super-heavy elements
Fermi neutron-induced (1939)
Rutherford transmutation (1919)
Bethe-Weizsäcker (1939)
Hauser-Feshbach (1952)
r-process (B²FH 1957)
ITER (1985)
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