99mTc Production in North America

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    99m

    Tc PRODUCTION PROCESSES: AN EXAMINATION OF PROPOSALS TOENSURE STABLE NORTH AMERICAN MEDICAL SUPPLIES

    Submitted by

    Margaret Cervera

    Department of Environmental and Radiological Health Science

    In partial fulfillment of the requirements

    for the Degree of Master of Science

    Colorado State University

    Fort Collins, Colorado

    Spring 2009

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    Introduction

    As a nation we are fearful of things we do not understand and producing a radioactive

    medical treatment from material used to create nuclear weapons is little understood and

    therefore generates great fear. The United States (US) currently relies on technetium-99

    metastable (99mTc) for a large number of medical diagnostic procedures with an ever

    increasing need, especially as the population ages. Supplies of99m

    Tc reach the United

    States via Canadas National Research Universal (NRU) reactor which is the sole large

    scale molybdenum-99 (99

    Mo) production facility in North America. This process

    currently depends upon multiple stages of cooperation that are susceptible to disruption at

    any time. The production of99mTc begins with shipping uranium-235 (235U) to Canada,

    irradiation of manufactured targets in a high neutron flux, removal of99

    Mo fission

    products from the reactor and radiochemical separation of the 99Mo. The 99Mo-99mTc

    generator can then be manufactured, shipped to a radiopharmacy and finally99m

    Tc is

    eluted for mixture to a final dosage form. Many agencies realize the urgent need for

    domestic production of99mTc but the ability to implement currently approved processes

    do not exist and changing the manufacturing process is a complex scientific and

    regulatory issue.

    For many people radioactivity in any form conjures visions of movie monsters,

    nuclear accidents such as Chernobyl and Three Mile Island and nuclear war. Society

    hears that weapons grade high enriched uranium (HEU) is being shipped around and out

    of the country and they are concerned; What if it is stolen? Will domestic fissile materials

    be used against us in an attack reminiscent of the Oklahoma City bombing or

    September 11th attacks? Will citizens be exposed to deadly radiation and require

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    evacuation from their homes? Will families face cancer as a result of any accidents

    involving transport or nuclear material? Where is the waste going to be stored and will it

    leak into my drinking water? In many ways these are valid concerns since accidents and

    acts of negligence have occurred with radioactive materials although generally with more

    limited consequences than many people believe. The technical aspects of generating

    99Mo, or any other radioisotope used for medical or research applications will be a

    challenge to present to the public in a way that will answer to concerns but not confuse

    people further. To a certain extent the publics concerns can be alleviated by education

    and openness. The purpose of this paper is to provide an insight into, and comparison of,

    the current state of production, the possible changes that are being considered and the

    infrastructure and scientific issues that will need to be resolved for the United States to

    supply this vital medical isotope.

    Importance and Use of99m

    Tc

    Tc-99m is the most commonly used medical isotope for medical imaging. It is

    involved in about 70% of all nuclear medicine procedures. Activities, in dosage form, for

    one brand, TechneLite, can range from just over 2 MBq/kg (0.05 mCi/kg) for pediatric

    thyroid imaging to 1110 MBq (30 mCi) for blood pool imaging of the heart (Bristol-

    Myers Squibb 2005). One of the highest use applications is for cardiac stress tests

    performed on over 40 million patients since 1991 (Bristol-Myers Squibb 2003). One

    brand of99mTc, Cardiolite, used in stress tests, generated sales of $304 million from

    January 2007 to September 2007, not including physician and additional treatment costs

    induced with each scan (Ghose 2008). Sales of99Mo, the precursor to 99mTc, are projected

    3

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    by the Society of Nuclear Medicine (SNM) to increase 15% over the next decade (Atcher

    2008) with Bio-Tech Systems market research predicting 7.5-9.4 % growth per year

    between 2006-2012, or 50-70% increase during that time (Committee 2009). Patent

    expiration and the entry of generics into the market are sure to have some effect on these

    projections.

    Diagnosing

    Brain

    Disorders >57,000 brainscans per year

    69,000projected in

    2010

    Treating Thyroid

    Cancer>608,000 thyroid

    imaging and therapyper year 652,000projected in 2010

    Imaging

    Lungs for

    Blood Clots>2,070,000lung scansper year2,350,000

    projected in2010

    Diagnosis and

    Monitoring of

    Cancer>818,200 cancer

    imagesper year

    2,053,000 projectedin 2010

    Scanning

    Bones for

    Infection>2,825,000bone scans

    per year3,255,000

    projected in2010

    Diagnosing

    Coronary Artery

    Disease>8,092,500

    cardiologyscans per year

    13,407,500projected in 2010

    Figure 1: Sample Medical Uses of99m

    Tc (Atcher 2008: data Bio-Tech Systems, images Journal of

    Nuclear Medicine)

    The absorbed radiation dose to specific organs of reference man (70 kg) is estimated

    by the manufacturer and is provided as a package insert with the formulation kit. Since

    99mTc is a gamma emitter the radiation dose is generally whole body although due to

    pharmakinetics localized organs will concentrate 99Tc at differing rates. Estimated

    absorbed doses (D) range from 1.8 mGy (breast) to 55.5 mGy (upper large intestine wall)

    due to the intravenous injection of 1110 MBq (30 mCi) of Cardiolite used for a stress

    4

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    test (Bristol-Myers Squibb 2003). For reference, the whole body limit for the public is 1

    mGy/y and to a radiation worker is 50 mGy/y. Both limits are in addition to that received

    from background and as a result of medical procedures.

    Tc-99m is an ideal radiopharmaceutical useful to medical applications because of

    an effective (inside the body) half-life (T1/2~ 6 h) long enough to complete a study with

    adequate concentrations remaining within the organ of interest, but also short enough to

    keep patient doses to a minimum. The short half life insures that a patient undergoing an

    outpatient procedure has cleared the99m

    Tc from all organs, by decay or excretion,

    approximately six hours from injection (Bristol-Myers Squibb 2003). The primary photon

    emitted, at 140 keV with 89% yield, is energetic enough to escape the body without

    significant attenuation (ICRP38 1999). The photon is detected by a gamma camera in

    which scintillators (plastic or NaI-Tl crystals depending upon brand) convert the energy

    of the photon into flashes of light which are converted by photomultiplier tubes into

    electrical pulses and are counted electronically.

    TcTcMo 99(gamma)IC)(orIT99mMeV1.2Edecaybeta99 max =

    T1/2:99Mo 67 hr

    99mTc 6 hr

    99Tc >105 yr (essentially stable)

    Figure 2: Decay of99

    Mo

    Due to its short half-life99m

    Tc cannot be produced directly since it will decay

    away in shipping before reaching the patient. Therefore it is eluted with sterile saline

    from a resin column containing its parent isotope 99Mo. Mo-99 is currently generated for

    use in the US as a fission product of uranium-235 (235U). The remainder of this paper will

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    discuss the status and challenges of producing99

    Mo on an adequate scale with a focus on

    the emerging and proposed process changes.

    Current Supply Processing

    Abbreviation Name235

    U Content

    NU natural uranium 0.7%

    LEU low enricheduranium

    20%

    HEU high enricheduranium

    > 20%

    HEU weapons grade 85%Table 1: Uranium Enrichment Grades

    The current system of producing 99Mo utilizes ~ 93% 235U as a requirement of the

    approved drug application on file with the Food & Drug Administration (FDA).

    Enrichment to 93% is not performed commercially in the US as HEU is generally used

    for nuclear weapon production. As a result the HEU used for 99Mo production is shipped

    from the Y-12 National Security Complex (Y-12) in Oak Ridge TN as it is removed from

    defense stockpiles (Mangusi 2000). HEU is then shipped to Chalk River Laboratories

    (CRL) in Canada to be manufactured into targets. Published Nuclear Regulatory

    Commission (NRC) records indicate shipments of HEU from the US to Canada for99Mo

    production totaling from 10-25 kg per year (NRC).

    At NRU MDS Nordion manufactures HEU targets, formed as pins of uranium -

    aluminum alloy within an aluminum cladding. These targets are then inserted via

    irradiation ports into the National Research Universal (NRU) reactor at CRL. The NRU

    reactor operates with neutron fluence (th) of approximately 21014 to 31014 n cm-2s-1.

    Up to 20 targets may be irradiated at any one time and can remain within the reactor for

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    five to seven days. The99

    Mo is generated as a fission product of235

    U and will occur in

    about 6% of all fissions (Reed 1953). Targets are monitored to determine removal at

    optimum times. The time of removal is determined based on the buildup of99

    Mo from the

    fission of235U. Due to an equilibrium, additional irradiation is not productive as the 99Mo

    will be lost due to decay as it is generated and therefore approximately 97% of the 235U

    remaining in the target will become waste (Committee 2009). The targets are removed

    after irradiation, allowed to cool in water for up to half a day, then are transferred to an

    associated hot cell facility (so named for its ability to handle the great heat and intense

    radiation of the targets) in shielded casks. Processing then must proceed quickly to

    minimize 99Mo losses due to radioactive decay. Approximately 1% of the generated 99Mo

    is lost to decay per hour after irradiation. For reference, the Cintichem reactor (which

    produced 99Mo in the US until 1989 when the reactor was shut down) typically yielded

    600 Ci of99

    Mo per target irradiated (Vandegrift 2007). Although processing equipment

    must be housed within a heavily shielded facility, the equipment itself is actually bench-

    scale and has a footprint similar to that of a large dining room table (Committee 2009).

    Ingrowth of Mo-99 vs Thermal Neutron Fission of

    U-235

    Mo-99

    U-235

    0 5 10 15 20 25 30

    t (days)

    Activity

    Figure 3: Buildup of99

    Mo in Reactor

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    Figure 4: Babcock & Wilcox hot cell facility (B&W)

    At the hot cell facility the cladding is punctured and gaseous fission products are

    removed, such as133

    Xe and131

    I, which are also valuable medical isotopes. Hot nitric acid

    dissolves the target assembly, forming a nitrate solution containing uranium,

    molybdenum and other fission products. This solution is then poured through an alumina

    column (Al2O3) that adsorbs the nitrates. The column is washed with additional nitric

    acid to elute excess uranium and other fission products but which leaves the molybdenum

    bound within the column matrix. The addition of sodium hydroxide will elute the

    purified99

    Mo (Saha 1998). This process typically yields recovery greater than 85-90%

    (Committee 2009). The removed 99Mo is shipped immediately to Mallinckrodt (dba

    Covidien) in Maryland Heights MO, or Bristol-Myers Squibb Medical Imaging (dba

    Lantheus Medical Imaging) inNorth Billerica, MA, where they then manufacture the

    generator. Manufacture includes adsorption of ammonium molybdate on Dowex-1

    anion exchange resin and washing with concentrated HCl removes any other impurities.

    The 99Mo is pH adjusted to form ammonium molybdate ((NH4)6Mo7O24) and is eluted

    from the column with dilute HCl (Saha 1998). The alumina column utilizes positively

    charged beads which adsorb the 99Mo as 99MoO42- (Zolle 2006). The column is

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    autoclaved for sterility. Additional purification and testing per pharmaceutical regulations

    is performed before the generator is packaged. The column has a higher affinity for the

    99Mo than the

    99mTc ensuring that the

    99mTc is preferentially eluted from the column.

    Elution of99Mo, or breakthrough, does occur. The amount of breakthrough is a quality

    control parameter of the manufacturer (Radioactivity 2009). The NRC regulates the

    amount of99

    Mo that may be given to humans to no more than 0.15 kBq99

    Mo per 1 MBq

    of99mTc (0.15 Ci 99Mo per 1 mCi 99mTc) and that, upon receipt of the generator, the

    concentration of99

    Mo in the first elution is verified to conform to the limit (Permissible

    2007).

    Due to the short half-life (~66 hour) of99Mo this process must take place quickly.

    Most nuclear medicine departments rely on continuous, multiple shipments of

    99Mo/99mTc generators per week to meet treatment demands. This supply chain is

    currently capable of supplying99

    Mo /99m

    Tc from reactor extraction to patient in less than

    48 hours (assuming no delays from any individual step). Industry practice currently sells

    bulk99Mo as six day curies which is nominally defined as the activity of the 99Mo in

    the generator six days after leaving the producer. Current weekly demand (2nd quarter of

    2008) is estimated at 6000 six-day-curies. This weekly demand equates to about 40,000

    Ci of99Mo at end-of-irradiation (out-of-reactor) (Robertson 2008).

    At the hospital or clinic a radiopharmacist will calculate the amount of99mTc that the

    decaying 99Mo has generated based on the transient equilibrium that exists between the

    two species. The 99mTc is eluted from the column with sterile saline (0.9% NaCl), as

    sodium pertechnetate (Na99m

    TcO4), and then is mixed with other reagents, according to

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    commercial kits like Cardiolite, into final patient dosage forms. The column is re-used,

    or milked, until all the 99Mo has decayed and the column is exhausted.

    Figure 5: Elution of Generator Column (generalized) (Sampson 1994)

    Figure 6: Decay-growth Relationship in a99

    Mo-99m

    Tc Generator (Saha 1998)

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    Figure 7: General Stages of99Mo Production from Irradiation to Patient. (Making 2008)

    Proposed changes to current supply processes

    The most pressing change to the development of a 99Mo source in the US is switching

    the targets from HEU to LEU, but other options are being considered as well. Other

    means of producing 99Mo include photo fission of235U, neutron activation of98Mo, and

    photo neutron interactions of100Mo . Construction of new reactors or conversion of

    existing reactors or the possible use of accelerators to meet increasing demand is also a

    focus of study as well as the use of alternate radionuclides or imaging protocols.

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    Using LEU Instead of HEU

    Converting existing reactors to LEU targets would significantly reduce the security

    concerns that surround the current supply process. The Schumer Amendment to the

    Energy Policy Act of 1992 restricts the export of HEU to research and test reactors, of

    which NRU is one, for any reason unless they can prove that they cannot use LEU as

    target material (Schumer 1992). Currently, NRU can only utilize targets manufactured

    using HEU due to the availability of waste storage capability and, mostly, FDA drug

    approvals, but research is progressing towards conversion to LEU targets. Clearly the

    change from HEU to LEU targets would seem to be simple, but there are technical and

    regulatory hurdles to overcome.

    Substituting LEU directly in place of HEU targets is possible. However, it would

    reduce the 99Mo yield to approximately 20% of that generated from the HEU. This is due

    to the reduced number of235

    U atoms available to fission (table 1). The lower yield can be

    overcome by irradiating five times more targets in the reactor. A reactor designated for

    99Mo production could be designed to have the space available to irradiate many more

    targets than current reactors can hold due to other user demands on them. Unfortunately,

    irradiating five times more targets would result in five times the volume of separation

    wastes which could quickly become a storage and disposal problem. Using LEU targets

    would also increase the generation of fissile 239Pu due to neutron capture by the higher

    proportion of238U. Generating 239Pu, a fissile and long-lived isotope, is also a national

    security concern. However plutonium is generally insoluble, and can therefore be

    separated from liquid wastes and ultimately be used to make mixed-oxide (MOX) fuel for

    nuclear power plants (see NRC Fact Sheet: Mixed Oxide Fuel).

    12

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    Figure 8: Production of239

    Pu Resulting from Neutron Capture by238

    U

    The increase in waste volumes is an important issue. If current target dissolution

    processes are maintained the waste storage facilities may not be able to accommodate a

    five-fold increase. Waste facility modification is one possibility for NRU however its

    also possible that in making certain changes they may not need to make that investment.

    It is possible that storage tanks are currently operating below capacity and by converting

    liquid wastes to solid form, waste storage will not be impacted (Committee 2009).

    Instead of irradiating more targets, the targets themselves could be altered to contain

    more LEU (increase the target volume). This approach would solve the issue of

    throughput in the reactor but could be limited by space restrictions in the reactor.

    Changing the composition of the target itself to contain more 235U by changing the

    density of the LEU target could also compensate for the reduced yield of99Mo. Current

    targets incorporate a uranium-aluminum alloy, with uranium density of approximately 1.6

    g/cm3. Converting to uranium metal could yield a higher density of uranium of about 8

    g/cm3. The change in density would approximate the mass of235U given the difference in

    enrichment (Committee 2009). Argonne National Laboratory (ANL) has been testing a

    LEU metal foil target within aluminum, nickel or zinc fission barriers that are

    encapsulated within a cylinder of aluminum cladding. Using foils, these targets, test

    irradiated in Indonesia, have been compatible with both acidic and alkaline dissolution

    processes (Vandegrift 1997). Commercial production using LEU targets is undergoing

    testing at the University of Missouri Research Reactor (MURR) which operates a

    maximum flux of 6 1014 n cm-2 sec-1(Committee 2009).

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    The main difficulty in utilizing LEU foils has been the method to manufacture the

    foils themselves. The LEU foils have been manufactured using three differing methods,

    by casting: pouring molten metal into molds, hot-rolling: heating the metal above its

    recrystallization temperature and then rolling it out to form sheets, or cold-rolling: rolling

    the metal out at room temperature to maintain its crystal structure. The casting method

    has produced irregular targets that, although useable, would make qualifying the

    uniformity of the targets more difficult and possibly more expensive to produce. Hot- and

    cold-rolling are both very labor intensive and therefore expensive to produce but result in

    better target uniformity (Committee 2009).

    After irradiation, a target of LEU or HEU must be chemically processed utilizing one

    of only two processes that are FDA approved: MDS Nordion or Cintichem. The

    (proprietary) MDS Nordion acid-dissolution process is in use for the isotope generated

    from NRU. The Cintichem process was purchased by the Department of Energy (DOE)

    from Cintichem Inc. upon the decommissioning of their Tuxedo NY reactor and is the

    focus of proposed modifications to convert to an LEU target for US supplies. According

    to available sources both processes are quite similar to each other, however a specific

    description of the MDS Nordion process is unpublished (Committee 2009).

    Ensuring that changes to chemical processing suitably achieve the removal of

    contaminating fission products is the focus of chemistry process research for LEU

    targets. The prime contaminants are isotopes of iodine (I), rhodium (Rh) and silver (Ag).

    Researchers from Argonne National Lab (ANL), and the Universities of Illinois and

    Texas have performed tests focusing mostly on the dissolution of the LEU foil targets in

    nitric acid as opposed to a mixture of nitric acid and sulfuric acid to avoid the generation

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    of sulfate species that can be corrosive in some storage situations (Gause 1982).

    Irradiation and processing of foils for the generation of99Mo has been tested in multiple

    countries with cooperation and funding from the International Atomic Energy Agency

    (IAEA). Testing of LEU foils and a modified Cintichem process with acid target

    dissolution are US, Indonesia, Poland, Chile, Korea, Libya, Pakistan, India and Romania

    (Goldman 2007). Results confirmed that utilizing LEU foils and a modified acid

    dissolution process are feasible alternatives to the current processes. Argentina has been

    producing99

    Mo utilizing LEU foils dissolved under a modified Cintichem process with

    alkaline conditions for their smaller scale domestic imaging needs. The Argentinean

    process was able to ultimately recover 92% of the available 99Mo but less than 10% of the

    contaminating131

    I. The131

    I is chemically reduced and therefore adsorbed onto the

    alumina column in addition to the 99Mo instead of being removed during purification

    (Vandegrift 2007). The differences in contamination purification efficiency that exist,

    dependant upon acid or alkaline dissolution, will likely determine the process ultimately

    chosen if LEU foils are used to generate US 99Mo supplies.

    It is not a requirement that a solid form of LEU is irradiated to generate usable 99Mo.

    A possible source of domestic99

    Mo is the Medical Isotope Production System (MIPS)

    plan proposed by Babcock & Wilcox (B&W). They have proposed to build an aqueous

    homogeneous reactor (AHR), also known as a solution reactor, which will utilize a LEU

    fuel salt dissolved in acid and water. Various solution forms are possible: uranyl nitrate

    (UO2(NO3)2), uranyl sulfate (UO2SO4), or uranyl fluoride (UO2F2). In this reactor the

    uranium in the solution is both reactor fuel and target material. This system would

    eliminate the necessity to manufacture or encapsulate a target and un-fissioned uranium

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    can be recycled back into the reactor instead of being removed as waste. The extraction

    process itself would not differ markedly from the existing adsorption to an alumina

    column that has already been in use. B&W has estimated that a reactor could generate

    approximately 1100 six-day Ci assuming a 26 hour processing time. They also have

    estimated a total waste volume of less than 5 m3 each year consisting generally of

    alumina column wastes (Reynolds 2007).

    Photo-fission of238

    U

    An accelerator can be utilized to generate99

    Mo by the photo-fission of the238

    U

    present in natural uranium. In this method a high intensity beam of photons is generated

    and directed at 238U (Freeman 2008). This results in nearly the same 6% fission yield for

    99Mo, however the cross section for

    238U is about 1000 times smaller than the neutron

    capture cross section for the fission of235U ( 600 barns for thermal neutron capture,

    37 barns for the production of99

    Mo assuming 6% fission yield) therefore a very large

    photon source would be required (Committee 2009).

    Using Molybdenum Instead of Uranium

    Eliminating uranium from the process is also a possibility by using other isotopes of

    molybdenum and converting them to99

    Mo. Four reactions are possible:98

    Mo(n,)99

    Mo

    (neutron activation) occurring inside a reactor, 100Mo(,n)99Mo (neutron emission),

    100Mo(p,pn)99Mo and 100Mo(p,2n)99mTc which require an accelerator.

    Neutron Activation of98Mo

    The activation of enriched 98Mo (natural molybdenum ~ 24% 98Mo) is currently in

    use by small producers in Kazakhstan and Romania. The reaction,98

    Mo(n,)99

    Mo

    (neutron activation), requires thermal (~ 0.025 eV) or epithermal (0.025 1.0 eV)

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    neutrons. Although this method does generate the desired99

    Mo, not all the98

    Mo is

    activated- analogous to the un-fissioned 235U from the MDS Nordion irradiations. This

    presents a problem in the purification to pharmaceutical specifications. Mo-99 produced

    in this way is not carrier-free, as it contains 98Mo that behaves chemically identical and

    acts as a contaminant. Thus, the 99Mo produced is termed low specific activity and would

    require larger generators, and by extension larger shielding around the generator, to

    produce the same activity required for a medical procedure. The FDA also limits the

    amount of99

    Mo that can breakthrough during the final dosage form elution process. The

    potential exists for increased elution of undesirable

    98

    Mo when formulating patient

    dosages which, beyond potential danger to a patient, limits the useful lifetime of the

    larger generator as it will need to be discarded due to breakthrough levels. As an aside,

    this method does not produce the secondary fission products that are of medical use,

    namely 131I and133

    Xe (Committee 2009).

    Ci/g106.3Bq/Ci107.3

    Bq/g1034.1

    )102.3*98(1.0)102.4*99(9.0

    104.17SA:Mo10%withMo

    Ci/g108.4Bq/Ci107.3

    Bq/g1076.1

    102.4*99

    104.17SA:free-carrierMo

    8

    10

    3

    195

    239899

    5

    10

    16

    5

    2399

    =

    =

    +

    =

    =

    =

    =

    ss

    s

    Figure 9: Specific Activity Effect of98Mo Contamination

    Accelerator Reactions of100

    Mo

    The accelerator produced methods explored do have merit. However all three would

    require extensive investment in accelerators that can generate very high intensity beams

    of protons (500 A) or electrons, to create photons, with sufficient energy to overcome

    the significantly smaller cross sections involved in these reactions. It has been calculated

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    that the100

    Mo(p,pn)99

    Mo reaction would require about 100 cyclotrons, assuming

    currently used cyclotron production values (Committee 2009).

    The final method,100

    Mo(p,2n)99m

    Tc, results in the direct production of99m

    Tc which

    has the significant disadvantage of time. Since the 99mTc has such a short half life (~6

    hours) any need to ship the generator over distances would reduce the usefulness to the

    end-user and, by extension, the patient.

    Other Challenges

    The current system of shipping HEU from Y-12 in Tennessee to NRU in Canada, and

    shipping 99Mo back to the US occurs with many points of contention and supplies are in

    almost constant jeopardy. Security concerning fissile materials that could be stolen and

    used as an improvised nuclear device (IND) or dirty bomb is a current fear concerning

    the use of HEU worldwide. Domestically, pharmaceutical companies must appeal to the

    Department of Energy (DOE) and the Nuclear Regulatory Commission (NRC) in order to

    secure defense stockpiled HEU from Y-12. Shipping itself is carried out under military

    supervision with permission from the Department of Transportation (DOT). All three

    agencies must grant approval for the raw material (HEU) to be shipped. Delays have

    occurred in the past due to reluctance of the various agencies to ship HEU to a private

    enterprise out of direct US control (Mangusi 2000). Legally, the Schumer Amendment to

    the Energy Policy Act of 1992 states that HEU cannot be exported from the US with very

    few exceptions allowed one of them being no approved alternative to the use of HEU

    such as that for generation of99Mo (10CFR110). As a result of these confounding factors,

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    periodic challenges to NRU and Cintichem (when in operation) regarding the transport

    HEU have arisen (Tilyou 1989).

    Another serious hurdle to overcome in the development of domestic production

    capability or changes to current processes is the approval for human use by the Food &

    Drug Administration (FDA). The production of any pharmaceutical, including medical

    radioisotopes, can only be performed according to a documented series of steps submitted

    and held by the FDA as a Drug Master File (DMF). Any changes to any step in the

    process will require an amendment to the DMF and subsequent approval by the FDA.

    The initial approval, such as would be required for a new manufacturer like B&W or

    MURR, includes a New Drug Application (NDA) which outlines all parameters for the

    manufacture of the drug (Brown 2005). Before any product can be given to patients, three

    complete production runs must be performed and evaluated for safety, efficacy and purity

    according to current Good Manufacturing Practices (cGMP) (21CFR210, 21CFR211).

    Even changes to an existing NDA or DMF requires an evaluation to ensure changes do

    not deleteriously affect drug safety, efficacy and purity. The product is tested against

    internal protocols but must conform to accepted pharmacopeial standards such as those

    covered in the United States Pharmacopeia (USP), the European Pharmacopeia (EP),

    Japanese Pharmacopeia (JP) or others. Some standard testing parameters are pH,

    concentration, radiochemical and radionuclide purity (Sodium 2009).

    Although extensive testing prior to process conversion should establish that 99Mo

    generated will perform no differently than the current process, the FDA will review all

    submitted data to determine the actual performance. This qualifying requirement adds

    considerable costs beyond infrastructure. These include protocol and system development

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    for the three qualification runs, raw materials testing, production costs of the three

    complete and typical-sized production runs, materials to complete the assembly of

    generators, final testing of the completed generators for all three runs and the costs

    associated with analyzing, compiling and completing the NDA. Each manufacturer will

    have to independently navigate this process which has been estimated to be at least

    $250,000 (Brown 2005). An FDA presenter to the National Academy of Science (NAS)

    suggested review lead times ranging from 4-18 months before approval although they

    could be extended significantly if FDA determined that human clinical trials would be

    required (Committee 2009).

    Figure 10: FDA Regulatory Process (adapted from Brown 2005)

    Another major stumbling block to domestic production is the capital investment that

    would be required. Estimates of costs and timelines vary extensively since no new reactor

    facilities or isotope separation facilities have begun construction in the US for over two

    decades.

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    Reactor NameConstruction

    Start

    Criticality

    Date

    Univ. Texas-Austin 1986 1992Watts Bar 1 1973 1996

    Comanche Peak 1 1974 1990Comanche Peak 2 1974 1993Seabrook 1 1976 1990Limerick 1 1974 1990

    Table 2: Recent US Reactors

    A facility dedicated to isotope production utilizing solid or liquid targets would need

    to construct a reactor in addition to hot cell and waste stream facilities. Commissioning a

    new reactor for isotope production is a lengthy process. Internationally, start of

    construction to commission of a reactor has been 6-8 years based on the ETRR2 in Egypt,

    FRM II in Germany and OPAL in Australia. An existing reactor, such as MURR, would

    need to create the capability to chemically separate the99

    Mo in an associated hot cell.

    Construction and commissioning of a new processing facility could take 3-5 years and

    has been estimated to cost $30 million to $40 million by the director of MURR, Ralph

    Butler (Committee 2009). Time estimates given are minimums and delays are always a

    possibility due to regulatory demands or design/construction changes (Committee 2009,

    Reynolds 2007).

    An example of the challenges to a new reactor facility is the Canadian MAPLE

    (Multipurpose Applied Physics Lattice Experiment) experience. Two reactors, MAPLE I

    and II, were planned and constructed to supply the worldwide 99Mo demand from one

    reactor and to utilize the other as a backup and research reactor. Costs projected to

    complete the MAPLE reactors (to replace the aging NRU) were estimated to be $130

    million. During the testing phase MAPLE I was discovered to posses a positive

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    temperature coefficient of reactivity. The temperature coefficient of reactivity, or

    multiplication factor, describes the number of neutrons available per generation per

    degree change in coolant temperature. A positive value indicates that there are more

    neutrons available as each fission generation progresses and the power of the reactor will

    increase as the temperature increases. A negative value indicates that there are fewer

    neutrons available for each subsequent generation and the power of the reactor will

    decrease as the temperature increases. The reactors were designed to have a temperature

    coefficient of reactivity of -0.12 mMW-1 but testing measured +0.28 mMW-1

    . Where

    is the effective multiplication factor and is dependant upon the absorption cross section

    of the fuel and moderator, the enrichment of the fuel (the MAPLE reactors were designed

    to utilize HEU fuel), the arrangement of the fuel rods and the coolant capabilities. This

    means that the inherent safety requirements of the reactor design were not met.

    Additional investigation could not determine the cause of the positive temperature

    coefficient of reactivity and in mid-2008 the project was cancelled (Magnus 2008).

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    The Four Factor Formula: = f p

    Symbol Name Meaning Dependence

    Reproduction

    Factor (eta)

    The number of fission neutrons produced per absorption in

    the fuel.

    fuel

    enrichment

    fThe thermalutilizationfactor

    Probability that a neutron that gets absorbed does so in thefuel material.

    compositionand geometryof fuel(reactordesign)

    pThe resonanceescapeprobability

    Fraction of fission neutrons that manage to slow downfrom fission to thermal energies without being absorbed.

    moderator/fuelratio (reactordesign)

    The fast fissionfactor

    cross sectionratio,moderator/fuelratio, fuelgeometry(reactordesign)

    Themultiplication

    factor

    -

    Table 3: The Four Factor Formula - Temperature Coefficient of Reactivity

    Babcock & Wilcox (B&W) assumes that five years will be required from conceptual

    design (which has begun) to commercial operation for their AHR. They have formed a

    partnership with a pharmaceutical company, Covidien, to assist with production and

    processing practice with B&Ws AHR design. An AHR has never been built at the

    proposed scale in the US and as such budget projections, based on experience, are

    lacking. The directors of MURR have also indicated their intention to commercially

    produce 99Mo and have solicited funding for studying the design and construction of

    facilities (Scully 2009).

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    A recurring theme with regard to developing any definite plans for the construction of

    domestic isotope production is securing capital from companies or federal budgets.

    Obtaining adequate funding is a major barrier to production. Government and private

    enterprise, including the medical community, seem to realize the importance of supplying

    99Mo. Unfortunately, funding for such projects will likely be hampered by the current

    economic crises and investments of such huge amounts of money may not be deemed

    appropriate or truly urgent until some recovery occurs. Waiting for funding will,

    obviously, put the ideal timelines out of grasp extending the time until the US can depend

    on its own isotope supply.

    Other Treatment Options

    There are other treatment options available to practitioners when supplies of

    99Mo/

    99mTc are limited. Since cardiac and bone scanning account for ~75% of

    99mTc

    applications the examination of alternate treatment modalities will focus on replacements

    in those areas. The main competitors to 99mTc are thallium-201 (201Tl), positron emission

    tomography (PET) utilizing rubidium-82 (82Rb), nitrogen-13 (13N) ammonia, or fluorine-

    18 (18

    F) as tracers and computed tomography (CT).

    The largest competitor to 99mTc for cardiac perfusion studies is 201Tl. Thallium-201

    can be used as a replacement for99mTc but they are often utilized in conjunction with

    each other. Thallium-201 is produced by irradiating a natural thallium target in the

    external beam of the 60 Brookhaven cyclotron with 31 MeV protons (Lebowitz 1975).

    The nuclear reaction is203

    Tl(p,3n)201

    Pb. The201

    Pb decays to201

    Tl in 9.4 hours. Thallium-

    201 is not considered an ideal isotope for imaging because it decays to mercury-201

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    (201

    Hg) and emits multiple characteristic x-rays resulting in lower quality images. It also

    tends to concentrate in the kidneys due to its longer half life (73 hours) resulting in a

    higher radiation dose to that organ than may be acceptable (Committee 2009).

    Figure 11: Decay and Emissions from Tl-201 (Lombardi 2006)

    The tracers used in PET include rubidium-82 (82

    Rb), which is cyclotron produced

    requiring 500 MeV protons. The nuclear reaction is 85Rb(p,4n)82Sr. The 82Sr (T1/2 ~ 26 d)

    decays to82

    Rb (T1/2 ~ 75 s) within a82

    Sr/82

    Rb generator (similar to the99

    Mo/99m

    Tc

    generator). Since the half life of the 82Rb is so short the generator is milked by

    continuous infusion directly into the patient. Use of82

    Rb with PET is limited by

    generator availability and insurance / Medicare reimbursement. Additionally, radiation

    doses to medical personnel who administer the tests can be significantly higher, possibly

    limiting the number of tests which could be performed at a center (Schleipman 2006).

    Ammonia with 13N is also used. This form of nitrogen has a 10 minute half life and

    therefore is made within a hospitals cyclotron. Obviously this limits treatment to

    geographical regions with cyclotron availability. Fluorine-18 (18

    F) is actually superior to

    99mTc for bone scanning however it has limited cardiac use since it is currently not a

    reimbursable treatment. The use of PET has increased dramatically, however it is

    estimated that the bulk of treatments with 99mTc are performed in private cardiology

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    not impacted negatively from the changes to their treatment plans, it is also likely that

    some were. A negative impact would be to health, insurance reimbursement, scheduling

    or trust in the abilities of their care providers.

    Additional challenges are constantly evolving. For example, in response to the

    National Academy of Science report, Medical Isotope Production Without Highly

    Enriched Uranium, released in January 2009, Representative Edward J. Markey (D-Mass)

    has stated his intent to introduce legislation to pressure change to eliminate HEU in the

    generation of99

    Mo and also to ensure supply reliability (Congressman 2009). As of this

    writing no legislation has been introduced. It is unknown how any additional legislation

    would impact the building of a significant source of99Mo in the US. More active and

    consistent support for changes to the supply chain comes from the IAEA and the global

    nuclear community who financially support and test the experimental changes explored

    throughout this paper.

    It seems that there is a favoring of converting worldwide production to the utilization

    of LEU with only minor consideration given to other production methods - although this

    may be more of a political drive rather than a technical necessity. Regardless, more time

    and money has already been invested in research to ensure that conversion to LEU will

    be successful. Given that LEU appears to be the preferred raw material for a domestic

    production facility I am intrigued by the possibilities of the AHR system. This reactor

    designs ability to use the uranium in uranyl nitrate both as target material and as reactor

    fuel appears economical to me. I also prefer its ability to essentially recycle the un-

    fissioned uranium back into the reactor as this could dramatically reduce the amount of

    waste that would require further processing or long-term disposal or security. I am

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    optimistic that the B&W / Covidien partnership can ultimately succeed in navigating the

    NRC licensing and FDA approvals to achieve their goal of producing a majority of the

    US demand for99m

    Tc.

    There are many hurdles to ensuring stable US supplies: security, economy,

    infrastructure and the technical changes to processing procedures in moving away from

    HEU. Ensuring that the supply can be achieved while ensuring homeland security and

    environmental safety is also important. Of ultimate importance however is supplying

    99Mo/

    99mTc to patients in a prompt and dependable manner because it is important to the

    health and longevity of the American population.

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    29

    Figure12:Q

    uickReview

    ofProcesses

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