The total energy released (Qtotal) in the decay of a 88226Ra nucleus from its ground state to the ground state of 86222Rn is given by the mass defect:
Δm=M(Ra)−M(Rn)−M(α)
Given values:
M(Ra)=226.005 u
M(Rn)=222.000 u
M(α)=4.000 u
Δm=226.005−222.000−4.000=0.005 u
Using 1 u=931 MeV/c2, the total Q-value is:
Qtotal=0.005×931 MeV=4.655 MeV
Now, consider the α-decay of 88226Ra at rest to an excited state of 86222Rn. Let Qα be the energy released in this step. By conservation of linear momentum, the momenta of the excited 86222Rn nucleus and the α-particle are equal in magnitude:
pRn=pα
The kinetic energy of the recoil 86222Rn nucleus is:
KRn=2MRnpRn2=MRnMαKα
Thus, the energy Qα shared between the kinetic energies of the α-particle and the recoil nucleus is:
Qα=Kα+KRn=Kα(1+MRnMα)
Given Kα=4.44 MeV, Mα=4.000 u, and MRn=222.000 u:
Qα=4.44×(1+2224)=4.44×(1+1112)=4.44×111113=4.52 MeV
The excitation energy E∗ of the 86222Rn nucleus is the difference between the total energy available and the energy released in the α-decay:
E∗=Qtotal−Qα=4.655 MeV−4.520 MeV=0.135 MeV
When the excited 86222Rn nucleus transitions to its ground state, it emits a γ-photon of energy equal to this excitation energy (since the nuclear recoil during photon emission is negligible):
Eγ=E∗=0.135 MeV=135 keV
Answer:
135