A property of atomic nuclei caused by the structural instability of some nuclei, resulting in the spontaneous transformation of unstable nuclei into more stable nuclei, with the emission of excess energy in the form of ionizing radiation
Radiation
Energy in motion, in the form of sub-atomic particles (protons, neutrons, alpha particles, beta-particles, positrons) or electromagnetic radiation (gamma rays, X-rays)
Sub-atomic particles
Emitted directly from the nucleus
Beta (β) particles: negative electrons (negatrons) or positive electrons (positrons)
Alpha (α) particles: +2 Helium nucleus (2p + 2n)
Travel only microns (alphas) or millimeters (betas) in any solid or liquid matter including living tissues, used primarily for therapy
Electromagnetic radiation (photons)
Emitted directly from the nucleus
Gamma (γ) rays: High energy/more penetrating
X-rays: Lower energy/less penetrating
Travel >> 1 cm in any solid or liquid matter including living tissues, used primarily for imaging/diagnosis
177Lu
A component of anti-cancer drugs Lutathera and Pluvicto
Pop Quiz 1
Iodine has an atomic number of 53. Calculate the neutron number of 131I.
Pop Quiz 2
Among the following group of radionuclides, identify those which are isotopes, isotones and isobars: 11 6 C, 10 5 B, 11 5 B, 11 4 Be
Determinants of nuclear stability
Size (atomic number Z)
Neutron to proton ratio (N/Z)
A BFCA has to form metal chelates with high thermodynamic stability or better kinetic inertness at 5 < pH < 7.5
Alpha (α) decay
Occurs only for large nuclei, Z > 90
α particles emitted by a particular radionuclide are monoenergetic and have a characteristic kinetic energy
α particles typically have kinetic energies of ~ 5 MeV
α emission does not alter N/Z ratio. A is decreased by 4 units, N – by 2 units and Z – by 2 units
Radionuclides
18Fluorine
11Carbon
89Zirconium
111Indium
99mTechnetium
With 6 hr half-life decays via IT to 99Technetium with 10^5 years half-life
The loss of radiometal would cause undesirable side effects by accumulation in nontarget organs
Decay constant
N=N0 e-λt, where N is the number of atoms at time t, N0 is the number of atoms at time 0, and λ is the decay constant for the radionuclide - it is the fraction of the atoms in a sample of that radionuclide undergoing radioactive decay per unit of time
Branching decays
e.g. 18F has 97% positron decay and 3% electron capture, so it λ = λ1 + λ2
Radioactivity
A= λN, where A is expressed in disintegrations per second (Becquerel (Bq), SI unit)
Radioactivity
A=A0 e-λt
Curie (Ci)
1 Ci= 3.7 x 1010 Bq
Half-life
T1/2 of a radionuclide is the time required for it to decay to 50% of its initial activity level
Half-life formula
T1/2 =0.693/λ
Average lifetime
τ = 1/λ, τ= 1.44 T1/2
Specific activity
Radioactivity of 1 g of the radioisotope, expressed in Bq/g. A=(0.693 x 6.023 x 1023)/(atomic weight of the radioisotope x T1/2), where 6.023 x 1023 is Avogadro's number. This formula should be used only for carrier-free radioisotopes, which do not contain any stable isotopes of the same element.
Pop up quiz
Calculate the specific activity of 1 g of 131Iodine with half-life of 8 days.
Bateman Equations
Needed when the product of radioactive decay (daughter) is also decaying. Examples: 99Molybdenum -> 99mTechnetium -> 99Technetium, 225Radium -> 225Actinium -> 221Francium -> 213Bismuth -> 209Bismuth.
Secular equilibrium
Parent is very long lived, and a daughter is very short lived, e.g. 225Actinium (9.9 days) and its daughter 213Bi (46 min). When A1 = A2, the parent and the daughter are in secular equilibrium.
Transient equilibrium
Parent half-life is longer than the daughter's half life, but is not infinite. A2/A1=T1/(T1-T2), tmax = [1.44T1T2/(T1 - T2)]ln(T1/T2). Example: 99Mo/99mTc.
Pop up quiz
Calculate the time when the maximum daughter activity is available for 99Mo/99mTc pair with the half-lives of 66 and 6 hours, respectively.
No equilibrium
When the daughter's half-life is longer than the parent's half-life, there is no equilibrium between them. Example: 131mTellurium with 30 hr half-life decays to 131Iodine with 8 days half-life.
Free radiometals may show a high toxicity (177Lu, 90Y, or 153Sm are "bone seekers" and would cause bone marrow damage)
Approaches to production of radionuclides
Traditional: Nuclear reactors
Particle accelerators
Alternative: Photonuclear reactions
Spallation sources
The BFC is often competing with natural chelators present in the blood stream like transferrin or serum albumin
Research Nuclear Reactors Worldwide and in Canada
Chalk River Reactor at the Canadian Nuclear Laboratories (Ontario) – decommissioned
McMaster Nuclear Reactor (Ontario)
École Polytechnique (SLOWPOKE-2) (Quebec)
Saskatchewan Research Council (SLOWPOKE-2) - decommissioned
Royal Military College of Canada (SLOWPOKE-2) (Ontario)
Neutron flux
The most important characteristic of a research nuclear reactor, measured in neutrons/cm2 x sec. To obtain radionuclides usable for radiopharmaceutical production, neutron flux needs to be > 10^13. McMaster Nuclear Reactor neutron flux is 10^14 neutrons/cm2 x sec
New way to produce radionuclides in commercial nuclear power plant reactors
1. New Isotope Production System at Bruce Power successfully produces first medical isotope
2. First-of-a-kind Isotope Production System continues to progress towards commercial, industrial-scale production of medical isotopes for cancer therapeutics
An international collaboration between Bruce Power, Isogen, and ITM Isotope Technologies Munich SE (ITM), announced today a milestone marking the first instance lutetium-177, a short-lived medical isotope, has been produced in a commercial nuclear power reactor.