Title: Introduction to Nuclear Medicine or Molecular Imaging
1Introduction to Nuclear Medicine or Molecular
Imaging
- Paul Benny
- Department of Chemistry
2History of Radiopharmacy
- Medicinal applications since the discovery of
Radioactivity - Early 1900s
- Limited understanding of Radioactivity and dose
31912 George de Hevesy
Father of the radiotracer experiment. Used a
lead (Pb) radioisotope to prove the recycling of
meat by his landlady. Received the Nobel Prize
in chemistry in 1943 for his concept of
radiotracers
4Early use of radiotracers in medicine
- 1926 Hermann Blumgart, MD injected 1-6 mCi of
Radium C to monitor blood flow (1st clinical
use of a radiotracer) - 1937 John Lawrence, MD used phosphorus-32
(P-32) to treat leukemia (1st use of artificial
radioactivity to treat patients) - 1937 Technetium discovered by E. Segre and C.
Perrier
5Early Uses continued
- 1939 Joe Hamilton, MD used radioiodine (I-131)
for diagnosis - 1939 Charles Pecher, MD used strontium-89
(Sr-89) for treatment of bone metastases. - 1946 Samuel Seidlin, MD used I-131 to
completely cure all metastases associated with
thyroid cancer. This was the first and remains
the only true magic bullet. - 1960 Powell Richards developed the Mo-99/Tc-99m
generator - 1963 Paul Harper, MD injected Tc-99m
pertechnetate for human brain tumor imaging
6Part 1 Characteristics of a Radiopharmaceutical
- What is a radiopharmaceutical?
- A radioactive compound used for the diagnosis and
therapeutic treatment of human diseases.
Radionuclide Pharmaceutical
7Radioactive Materials
- Unstable nuclides
- Combination of neutron and protons
- Emits particles and energy to become a more
stable isotope
8Radiation decay emissions
- Alpha (a or 4He2)
- Beta (b- or e-)
- Positron (b)
- Gamma (g)
- Neutrons (n)
9Interactions of Emissions
- Alpha (a or 4He)
- High energy over short linear range
- Charged 2
- Beta (b- or e-)
- Various energy, random motion
- negative
- Gamma (g)
- No mass, hv
- Positron (b)
- Energy gt1022 MeV, random motion
- Anihilation (2 511 MeV 180)
- Negative
- Neutrons (n)
- No charge, light elements
10Half Life and Activity
- Radioactive decay is a statistical phenomenon
- t1/2
-
- l decay constant
- Activity
- The amount of radioactive material
11Why use radioactive materials anyway?
- Radiotracers
- High sensitivity
- Radioactive emission (no interferences)
- Nuclear decay process
- Independent reaction
- No external effect (chemical or biochemical)
- Active Agent
- Monitor ongoing processes
12Applications in Nuclear Medicine
- Imaging
- Gamma or positron emitting isotopes
- 99mTc, 111In, 18F, 11C, 64Cu
- Visualization of a biological process
- Cancer, myocardial perfusion agents
- Therapy
- Particle emitters
- Alpha, beta, conversion/auger electrons
- 188Re, 166Ho, 89Sr, 90Y, 212Bi, 225Ac, 131I
- Treatment of disease
- Cancer, restenosis, hyperthyroidism
13Ideal Characteristics of a Radiopharmaceutical
- Nuclear Properties
- Wide Availability
- Effective Half life (Radio and biological)
- High target to non target ratio
- Simple preparation
- Biological stability
- Cost
14Ideal Nuclear Properties for Imagining Agents
- Reasonable energy emissions.
- Radiation must be able to penetrate several
layers of tissue. - No particle emission (Gamma only)
- Isomeric transition, positron (b), electron
capture - High abundance or Yield
- Effective half life
- Cost
15Detection Energy Requirements
- Best images between 100-300 KeV
- Limitations
- Detectors (NaI)
- Personnel (shielding)
- Patient dose
- What else happens at higher energies?
- Lower photoelectric peak abundance, due to
the Compton effect
Cs-137 decay (662 KeV)
Energy ?
16Gamma Isotopes
- Radionuclide T1/2 g ()
- Tc-99m 6.02 hr 140 KeV (89)
- Tl-201 73 hr 167 KeV (9.4)
- In-111 2.21 d 171(90), 245(94)
- Ga-67 78 hr 93 (40), 184 (20), 300(17)
- I-123 13.2 hr 159(83)
- I-131 8d 284(6), 364(81), 637(7)
- Xe-133 5.3 d 81(37)
17Positron Emission Tomography
- b slows to thermal energies two 511KeV gammas
rays emitted approximately 180 to each other - Coincidence detection
- b travel some distance from the initial site
- Cyclotron produced
- Sharp images
- Quantitative
- Short Half Lives
18PET Isotopes
- Nuclide T1/2 Production
- Carbon-11 20.4 min 10B(d,n)11C
- Nitrogen-13 9.96 min 12C(d,n)13N
- Oxygen-15 2.05 min 14N(d,n)15O
- 16O(p,pn)15O
- 12C(a,n)15O
- Fluorine-18 110 min 18O(p,n)18F
- Copper-64 12.7 hrs 64Ni(p,n)64Cu
19ImagingPET vs. SPECT
- More complex and larger molecules
- Less quantitative
- Longer half lives
- Available world wide
- Less expensive
- No special production equipment needed
- Biologically useful isotopes
- 11C, 13N, 15O, 18F
- More Quantitative (b)
- Very short T1/2
- Very expensive
- On site cyclotron
20Radiopharmaceuticals for Therapy
- Similar to imaging requirements
- Effective half life, high abundance, availability
etc. - Particle emitters
- a, b, auger, amd conversion electrons
- Particle energy
- Is higher better? Linear Energy Transfer (LET)
- Additional g rays help with determining
localization via imaging methods.
21Some Radionuclides for Therapy
- Radionuclide T1/2 Particle (MeV)
- Re-186 3.8 b- (1.07)
- Re-188 17 hrs b- (2)
- I-131 8 d b- (2)
- P-32 14.3 d b- (1.7)
- Sr-89 50.6 d b- (1.43)
- Sm-153 1.9 d b- (0.81)
- Bi-212 1 hr a (6.051)
22Therapeutic Radiation Dose
- External cell receptors vs. DNA binding agents
- Distance does matter
- Ionization and angle of interaction
- Probability of DNA damage increases as distance
decreases
23DNA Damage in Radiotherapy
- Ionization
- Direct and Indirect
- Alpha, beta, Auger electron, internal conversion
- Free Radical Induction
- (R., OH., HOO.)
- Irreparable damage to DNA through strand cleavage
- Double and single strand breaks
- Base pair mutation
- Therapy Goal Induce cellular apoptosis
24How do you prepare radioisotopes?
- Site produced
- Reactor or cyclotron
- Limited by half life, facilities,
- Limited Shipping distance
- Generator system
- Portable system
- Reusable
25Cyclotron
Reactor
26Production of Radionuclides
WSU Reactor
- Nuclear Reactor (neutrons)
- Fission of U-235
- Produces neutron rich radioisotopes
- Alpha, Beta, gamma decay
- (n, g) reaction
- Cyclotron (charged particles)
- Proton rich
- Positron, electron capture
- (p,n), (d,n) reaction
- most common
Washington University St. Louis, MO
27A generator facilitates the separation of two
radionuclides (parent and daughter) from each
other to yield a useable radioisotope (daughter)
for nuclear medicine studies.
- Transient equilibrium
- T1/2 daughter is less than 10 half lives than the
parent - Ad ld Ap e-lpt/(ld-lp)
- Secular equilibrium
- T1/2 of the parent much greater than 10 half
lives of the daughter. - Activity at equilibrium (Ap Ad)
- Cs-137 (T1/2 30 y) and Ba-137m (T1/2 2.5 min)
28Ideal Characteristics for a Generator
- Utilizes chemical characteristics of the parent
and the daughter radionuclide. - Output sterile and pyrogen free
- Biological pH
- Low radiation dose (Shielding)
- Inexpensive.
- Easy to produce.
- Simple elution method
- Reasonable half life of parent and daughter
Parent Daughter
Daughter
2999mTc The workhorse of Nuclear Medicine Industry
- Imaging Radionuclide
- gt90 FDA approve imagining agents are 99mTc
- Versatile chemistry
- Ideal Nuclear characteristics
- T1/2 6.02 hr
- Gamma, 140 KeV (89)
- Internal conversion (11)
- Energy vs. effectiveness of the decay
- Availability (generator)
- 99Mo?99mTc
30Mallinckrodt/Tyco 99mTc Generator
- High specific activity 99Mo from 235U fission
- Solid phase
- Alumina
- Liquid phase
- 0.9 saline
- Generator easy to use
- Reliable separation
31(No Transcript)
32Common radiochemical generators
- Eluants
- 1. 0.9 NaCl
- (99Mo ? 99mTc)
- (82Sr ? 82Rb)
- 2. 0.05 N HCl
- (113Sn ? 113mIn)
- 3. O2 (81Rb ? 81mKr)
-
- 4. 1 N HCl 68Ge ? 68Ga)
- Column Materials
- 1. Alumina (99Mo ? 99mTc)
- Zirconia
- (113Sn ? 113mIn)
- Cation exchange resin
- (81Rb ? 81mKr)
- 4. Anion exchange resin
- (62Zn ? 62Cu)
- Stannic Oxide
- (82Sr ? 82Rb)
33Effective Half life (Radio and biological)
- Nuclear Decay (T1/2)
- Inherent statistical decay of the nuclide
- Biological T1/2
- Uptake/washout of the radiopharmaceutical
- Equilibration
- Decomposition
- Pairing of biological and radionuclidic half
lives is imperative to optimize effectiveness of
the drug.
34High target to non target ratio
- Lower activity require for detector statistics
and visualization of target tissue. - Low dose to non target tissues
- Bone Marrow, gastro intestine
- Decreased probability of organ overlap
35How do agents localize at target tissues?
- Method of Localization
- Active transport
- Phagocytosis (Liver uptake)
- Capillary blockade
- Simple/Exchange diffusion
- Compartmental Localization
- Chemisorption
- Antigen/Antibody reaction
36Several Types of Radiopharmaceuticals
Cocaine
- 1) Radioactive atom
- 131I- ,201Tl, 81mKr
- 2) Radioactive compound
- I, C, or transition metals.
- Covalent or coordination bond.
Ritalin
37Methods of Labeling
- Direct labeling
- Non specific binding
- Antibodies, red blood cells
- Site specific
- Iodination (Tyr) , Methylation (amine, cys)
- Chelate
- Metal Ligand coordination complex
- Bifunctional Chelate
- Normal chelate with biological targeting agent
38Chelate Groups
- Mixture of coordination donor atoms
- N, O, S, P, etc.
- Geared to metal and oxidation state
- Monodentate to multi-dentate
- 1-8 coordination donors
- Variety of coordination modes
- Fac, mer, planar, equatorial, tetrahedral,
asymmetric
39Example Chelate Systems
- Various denticity (1-8)
- Variations of donor atoms (N,S,O,P)
- Metal chelate ring size
- Complex stability
- Combination of multiple ligands
- 22, 31,32
40Biological Target Design
Targeting Agent
Radionuclide
Biological Target
- Target a specific biological function
41Target Specific Radiopharmaceuticals
Biological target
- Targets (unique features)
- Cell surface receptors
- Transport mechanisms
- Proteins
- DNA/RNA
- Targeting Molecules
- Peptides
- Peptide mimics
- Nucleotides
- Small molecules
- Antibodies
42Types of Radiopharmaceuticals
- Small molecule
- Fast circulation
- Good specificity
- Less than 1,000 daltons
- Metal chelate considerable of mass
- Large molecule
- Slow circulation
- Excellent specificity
- Usually contains a biologically active motif
- Antibodies or fragments, B-12
- Metal chelate insignificant of mass
43Peptide Labeling
- Small peptides for specific receptors
- Easy to produce
- Greater number of variations to optimize the
system - Faster circulation through the body
- Maintains specificity.
- Better clearance
- Via kidneys rather than liver
Somatostatin
44Labeling Antibodies
- High specificity to an antigen or binding site
- Large molecular weight
- 50,000 daltons
- Labeling
- Direct non specific method (131I)
- Bifunctional chelate
- Mab fragments
- (F(ab)2, Fab)
- Similar immune response to Mab
Mab
F(ab)2
Fab