pet radionuclides production cyclotron selection and … · 1 pet radionuclides production...

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1 PET Radionuclides Production PET Radionuclides Production Cyclotron Selection and Location Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental Diagnostic Imaging, The University of Texas MD Anderson Cancer Center Houston, TX 1. Cyclotron Selection a. Nuclear Reactions b. Production Methods c. PET Radionuclides d. Selection Criteria e. Radionuclide Production Yield 2. Cyclotron Site a. Large Vault Design b. Self-Shielded Option c. Facility Layout 3. PET Radionuclides Production a. Gas Targets b. Liquid Targets c. Solid Targets α, 3n α, 2n 3He, n α, n p, n p, γ d, n 3He, np α, np t, n 3He, p p, t p, pn γ, n n, 2n Original Nucleus n, n d, p n, γ t, np t, p p,α n, t γ, np n, d γ, p n, p t, 3He Displacement Caused by Nuclear Bombardment Reactions d, α n, np t, He n, α n, n 3He n, 3He n, pd p n Charged Particle (Accelerator) Neutron Irradiation (Reactor) Radionuclides Production Stars Formation Cosmic Rays Nuclear Reactor Cyclotron Cyclotron Accelerator

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Page 1: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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PET Radionuclides ProductionPET Radionuclides Production

Cyclotron Selection and LocationCyclotron Selection and Location

Carlos Gonzalez Lepera, Ph.D.CYCLOTOPE and

Experimental Diagnostic Imaging,The University of Texas MD Anderson Cancer Center

Houston, TX

1. Cyclotron Selection

a. Nuclear Reactionsb. Production Methodsc. PET Radionuclides d. Selection Criteriae. Radionuclide Production Yield

2. Cyclotron Site

a. Large Vault Designb. Self-Shielded Optionc. Facility Layout

3. PET Radionuclides Production

a. Gas Targetsb. Liquid Targetsc. Solid Targets

α, 3nα, 2n

3He, nα, n

p, np, γd, n

3He, np

α, npt, n

3He, p

p, tp, pnγ, n

n, 2n

OriginalNucleus

n, n

d, pn, γt, np

t, p

p,αn, t

γ, npn, dγ, p

n, pt, 3He

Displacement Caused by Nuclear Bombardment Reactions

d, α n, npt, He

n, αn, n 3He

n, 3Hen, pd

p

n

Charged Particle (Accelerator)

Neutron Irradiation (Reactor)

Radionuclides Production

Stars FormationCosmic Rays

Nuclear Reactor

CyclotronCyclotron

Accelerator

Page 2: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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Common PET RadioisotopesCommon PET Radioisotopes

Radioisotope Half-life Decay (%) β+ Endpoint (MeV) Principal Nuclear Reactions

1111CC 20.3 min β+ 99.8, EC 0.2 0.961 14N(p,α)11C

1313NN 9.96 min β+ 100 1.190 16O(p,α)13N

1515OO 122 sec β+ 99.9, EC 0.1 1.72314N(d,n)15O15N(p,n)15O

1818FF 109.8 min β+ 96.9, EC 3.1 0.63518O(p,n)18F

FF 109.8 min β 96.9, EC 3.1 0.635 20Ne(d, α)18F

61Cu 3.41 hr β+ 62, EC 38 1.20560Ni(d,n)61Cu61Ni(p,n)61Cu

62Cu (gen.) 9.73 min β+ 97.8, EC 2.2 2.934 63Cu(p,2n)62Zn(9.1 hr) → 62Cu

64Cu 12.7 hr β+ 19, EC 41, β- 40 0.657 64Ni(p,n)64Cu, 64Zn(n,p)64Cu

82Rb (gen.) 75 sec β+ 96, EC 4 3.35 85Rb(p,4n)82Sr(25 d) → 82Rb

86Y 14.7 hr β+ 34, EC 66 1.248, others 86Sr(p,n)86Y

124I 4.15 d β+ 25, EC 75 1.533, 2.134 124Te(p,n)124I

Cyclotron Selection Criteria

Purpose Commercial Distribution

Distribution & Research Clinical Research Pre-Clinical

Research

Radionuclide 18F11C, 13N, 15O, 18F, solid

11C, 13N, 15O, 18F, solid

11C, 15O, 18F

Activity ~ 10 Ci/batch > 1 Ci/batch ~ 1Ci/batch < 1 Ci/batch

$ $

Particles H- H-, D- H-, D- H-

Energy ≥ 15 MeV ≥ 15 MeV ≥ 15 MeV ≥ 7 MeV

Shielding options: Self + Vault (~30 cm concrete)Vault (~ 200 cm concrete)

Long term investment >10 years Long term needs

Radionuclide Production YieldsRadionuclide Production Yields

Disintegration Rate: D = N . λΑ N : Number of atoms(Activity) λA : Probability of decay

λA = ln(2)/T1/2

Bateman’s equation (balance) for growth of daughter radionuclide B from parent A

( ) ( )( )tBAB

ABeAB ⋅−−−⋅=⋅ λλ

λλλλλ 1( ) ( )

ABAB − λλ

A : Number of target atoms. A >> 1λA: Probability of transforming target atom A into B λA<<1The product A.λA remains finite.

λA < < λB⇒ ( )tAB

BeAB ⋅−−⋅=⋅ λλλ 1

Beam Targetx1 x2

I

Probability of transforming atom A into B

( )( )∫∑ ⋅⋅=⇒⋅⋅= 2

1

2

1

)(E

EA

x

xA dE

dxdEEIdxxI σλσλ

E1 E2

Page 3: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

3

( ) ( )( )∫⋅

⋅⋅−=⋅ ⋅−

th

i

B

E

E

AtB dE

dxdEE

MNeIB σρλ λ1

Radionuclide Production YieldRadionuclide Production Yield

Yield (mCi)

Build-up (irradiation time)

Saturation Yield (mCi/μA)

(I) Beam Current (μA)

BλB = I (1- e-λΒt) NAρ / M σ(E) dE/(dE/dX)

0 6

0.7

0.8

0.9

1

Irradiation Build Up

0

0.1

0.2

0.3

0.4

0.5

0.6

0 1 2 3 4 5

Half-life

Fact

or

BλB = I (1- e-λΒt) NAρ / M σ(E) dE/(dE/dX)

18O(p,n)18F Cross Section

400

500

arn)

1 mbarn = 10-27 cm2

0

100

200

300

0 5 10 15 20

Energy (MeV)

Cro

ss S

ectio

n (m

ba

BλB = I (1- e-λΒt) NAρ / M σ(E) dE/(dE/dX)

18O(p,n)18F Saturation Yield

200

250

300

/ μA

)

0

50

100

150

200

0 5 10 15 20

Energy (MeV)

Satu

ratio

n Y

ield

(mC

i /

Page 4: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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Production EfficiencyProduction Efficiency

How many protons per produced 18F atom are needed?18O(p,n)18F

Protons Energy [MeV]

Yield*[mCi/μA]

18F at EOB [mCi]

Protons/18F

10 5 120 950 170010.5 120 950 1700

18 200 1583 1020

Irradiation conditions : 25 μA x 60 min

* Typical production yields using >95% enriched 18O-Water

Ernest Orlando Lawrence and M. Stanley Livingston

Holifield Radioactive Ion Beam Facility – Oak Ridge ,TN

25 MV Terminal Building

Comparative size for electrostatic accelerator with similar final proton energy as 40 MeV cyclotron

UT Houston UT Houston –– Scanditronix MC40Scanditronix MC40

Page 5: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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TRIUMF

TR

500

MeV

CYCLOTRON MENUCYCLOTRON MENU

Sizes: Small (PET): K(p) < 19 MeV self-shielded option

Medium (SPECT): K(p) < 30 MeV vault required

Large (Therapy): K(p) > 30 MeV up to few hundred MeV

Flavors: Ion Positive Negative (p, d only)Ion Source Internal External

Magnet Conventional Superconducting

Plane Horizontal VerticalShielding Self VaultParticles Single Multiple (p,d,α,He3)Energy Fixed Variable (steps-cont.)

Siemens Eclipse HP

11 MeV protons

60 μA (x2)max. current

MAX. POWER: 660 W (x2)

GE PETtrace

16 MeV protons

8 MeV deuterons (option)

60 μA max. current

MAX. POWER: 960 W

Page 6: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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GE PETtrace Self-Shielded

18 MeV protons

9 MeV deuterons

150 μA max. current

MAX. POWER: 2700 W

IBA Cyclone® 18/9 -HC

ACS TR 19/9

19 MeV protons

9 MeV deuterons

>300 μA current

MAX. POWER: ~ 6000 W

Production Capacity

8000

10000

12000

14000

eld

(mC

i)

100 μA100 μA

(1 target – 2 hours)

0

2000

4000

6000

0 5 10 15 20

Energy (MeV)

18F

Yie

60 μA

60 μA

60 μA

Page 7: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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Large Vault (~190 cm walls)

Shielding (neutrons)

NCRP 144

Reinforce floor

Beam direction

Negative pressure

Conduits – Power and utilities

Trenches – Product delivery

Corner Pit – Decay in storage

Power supply room

Support room

Control room – Vault door

Work bench – targets service

Product distribution valves

Self-shielded (~30 cm walls)

Shielding (neutrons)

NCRP 144

Reinforced floor

Beam direction

Negative pressure

Conduits – Power and utilities

Trenches – Product delivery

Corner Pit – Decay in storage

Power supply room

Support room

Control room – Vault door

Work bench – targets service

Product distribution valves

RF DeesTarget Holder

Extractorload lock

Open Cyclotron All parts requiring maintenance can be isolated from the cyclotron vacuum

Page 8: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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Beam Lines

Page 9: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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Extraction Foil

Target holder accepts four targets on either side of cyclotron intovacuum sealed mount.

Target Holder mountedto cyclotron. Positionedwith mechanical bellows

adjustment

Page 10: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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1111CC Nuclear Reaction: 14N (p,α)11C

Target Material- Aluminum

τ = 20.3 min

N2 + 11CO2beam

N2

UHP N2

Trapping 2

11CO2

Labeling

Specific Activity: 1-10 Ci/μmol (10-3)Yields

Purification

Final Product

Target : ~ 1 CiTrapping: > 90%Labeling: ~ 50%Purification ~ 50%

11CO2

Commercial Distribution: NONO

Single DoseSingle Dose

1313NN Nuclear Reaction: 16O (p,α)13N

Target Material- Aluminum

τ = 9.96 min

He gas (500 psi)

H2O + EtOH (trace)beam

Water Cooling

Specific Activity: NCAYields

Purification

Target : 500 mCiLabeling: In targetPurification ~ 95%

Commercial Distribution: Very LimitedLimited

13N-Ammonia

Final Product

Single/Dual DoseSingle/Dual Dose

1515OO Nuclear Reaction: 14N (d,n)15O

Target Material- Aluminum

τ = 2.03 min

UHP N2 +5% H2

N2 + H215Obeam

N2Trapping

2

H215O

Purification

Specific Activity: NAYields

Purification

Final

Product

Target : 500 mCiTrapping: ~ 80%Conversion: ~ 40-80%Purification ~ 98% Commercial Distribution: NONO

H215O

C [15O]

O [15O]Conversion Conversion

Single DoseSingle Dose

Page 11: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

11

1818FF Nuclear Reaction: 18O (p,n)18F

Target Holder Material- Titanium- Silver- Niobium- Tantalum

τ = 109.8 min

He gas (500 psi)

H218O ( > 95%)beam

Water Cooling

H218O recover K222 + K2CO3

> 1 kW Power Dissipation!

Specific Activity: NCAYields Target : 5-10 Ci

Trapping: > 95%Labeling: 30-60%Purification ~ 95% Commercial Distribution: YES !YES !

2

18F trap

Purification

18F Reaction Vessel Final Product

BatchBatch

2 3

PrecursorSynthesis

Unit

6161CuCu Nuclear Reaction: 60Ni (d,n)61Cu - nat.Ni : 60Ni (26.1%)

Target Material- Aluminum

τ = 3.41 hr

beamWater Cooling

Ni waste/recover T ~ 90 ºC HCl

Beam Power > 6 kW

Specific Activity: NCAYields Target : 100 mCi

Trapping: > 98%Labeling: 30-80%Tracers: 6161CuCu--ATSMATSM Commercial Distribution: YESYES

Ion Exchange Resin

Final Product

BATCHBATCH

H2O/HCl

Target Dissolving

124124II Nuclear Reaction: 124Te (p,n)124I

Target Material- Aluminum

τ = 4.4 d

beamWater Cooling

T ~ 670 ºC

Platinum or Tantalum substrate

124TeO2/Al2O3

Specific Activity: > 30 Ci/μmolYields Target : 200 mCi

Trapping: ~ 80%Labeling: ~50%Tracers: 124124II--mab/FIAUmab/FIAU Commercial Distribution: YESYES

NaOH Trap

Final Product

BATCHBATCH

H2O

Dry Distillation

O2

Class 100Mini Cells

Page 12: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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Dual FDG Production Units

Laminar Flow Dispensing Hot Cell

Dose DispensingPotential New Tracers Primary Application

F18-Acetate Oncology/Cardiology

F18-Fluorodopa Neurology -Oncology

F18-FLT Oncology –DNA marker –Cell Proliferation

C11 – PIB Detection Alzheimer’s disease (F18)

C11 – Acetate Heart/Prostate

FDA Approved:FDA Approved:

1818F[NaF]F[NaF]1818F[FDG]F[FDG]1313NN--AmmoniaAmmonia8282RbRb

C11 – Palmitate Fatty Acid Metab – Heart

C11 – Tracers Brain Receptors

I124 – MoAb Oncology/Diag.-Treatment

Cu-61/64 ATSM Hypoxia

Zn62/Cu62 Generator Heart

Page 13: PET Radionuclides Production Cyclotron Selection and … · 1 PET Radionuclides Production Cyclotron Selection and Location Carlos Gonzalez Lepera, Ph.D. CYCLOTOPE and Experimental

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FDG Fluoroacetate

Thank youy