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Synchrotron
Radiation in Cancer Radiotherapy: Search and Destroy
Brenda Laster and Gad Shani
Departments of Biomedical Engineering and Nuclear
Engineering
Ben Gurion University of the Negev
Beer Sheva 84105 Israel
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The
objective of patient treatment planning protocols in cancer radiotherapy
is t
o deposit maximum energy per gram of tumor and minimize the dose
to surrounding normal tissues. However, within the tumor treatment
volume, only the cellular DNA, whose mass is merely 0.25% the mass
of the entire cell, has been identified as the critical target for
killing the cell with radiation. Therefore, the probability that the
quanta of energy emitted by photons will interact and be absorbed
at the DNA target site is e
xtremely small. One approach that can be
taken to increase the efficacy of the radiation is to introduce high
Z atoms into the DNA. These atoms have a higher probability for absorbing
radiation than that of the ordinary biological atoms (C, O, H, and
N). Furthermore, when activated by photons whose energies are suitable
for inducing a photoelectric effect in the atom, the emission of low
energy, short range Auger electrons,
can act like an energy sink directly
in the DNA. These electrons increase the effective radiation dose
to tumor while sparing surrounding normal tissues. Auger Electron
Therapy (AET) takes this approach in an attempt to improve cancer
radiotherapy.
AET utilizes a drug to transport and attach high Z atoms to tumor
cell DNA, and photons whose energies are suitable for inducing a photoelectric
effect in the atoms to impart dense, clustered ionization directly
at the critical target and significantly increase the probability
of non-repairable, lethal damage to the tumor cell. This binary approach
to cancer treatment can avail itself of either synchrotron radiation
or implanted brachytherapy seeds as the sources of radiation, depending
upon the required energy for activating the high Z atom.
S
ynchrotron radiation is an ideal source for use in AET because photon
energies can be precisely tuned to the absorption edges of the various
atoms to meet the requirements for the induction of a photoelectric
effect, provided that the activating energy is capable of penetrating
the body to the depth of tumor. In those cases where the activating
energy is too low to achieve penetration, the interstitial implantation
of radioa
ctive brachytherapy seeds directly into the tumor can be
applied. The therapeutic gain from the implanted radiation sources,
in combination with the DNA-localized high Z atom, can then be predicted
through experimentation with synchrotron radiation. X-ray micrography
techniques using synchrotron radiation can also be used to search
for and identify the intracellular localization of the high Z atoms
within the cell. In previo
us studies at the National Synchrotron Light
Source at the Brookhaven National Laboratory, V-79 Chinese hamster
cells were irradiated with monochromatic photons above (28 keV) and
below (27.8 keV) the K absorption edge of indium (27.9 keV). Resulting
cell survival curves showed that Auger electron emission in indium
enhanced the radiation dose by a factor of ~2 compared to cells without
indium. A factor of >1.5 was obtained
in recent in vivo studies after
an indium-labeled porphyrin, InTMPyP, was administered following the
implantation of 125I brachytherapy seeds (average energy 28 keV) into
the B16 murine melanoma born on the flank of C57 Blas mice.
These results validate the fine-tuning capabilities of synchrotron
radiation as a tool for predicting the therapeutic advantage that
could be achieved in binary systems where
drug/radiation combinations
are exploited for improving cancer radiotherapy. They also demonstrate
the potential of synchrotron radiation as a clinical instrument for
activating atoms such as gadolinium or platinum whose higher activation
energies can achieve intracorporeal penetration.
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