There are two major medical applications of ion accelerators. One is a production of short-lived isotopes for radionuclide imaging with positron emission tomography and single photon emission computer tomography. Generally, a combination of a source for negative ions (usually H- and/or D-) and a cyclotron is used; this system is well established and distributed over the world. Other important medical application is charged-particle radiotherapy, where the accelerated ion beam itself is being used for patient treatment. Two distinctly different methods are being applied: either with protons or with heavy-ions (mostly carbon ions). Proton radiotherapy for deep-seated tumors has become widespread since the 1990s. The energy and intensity are typically over 200 MeV and several 10(10) pps, respectively. Cyclotrons as well as synchrotrons are utilized. The ion source for the cyclotron is generally similar to the type for production of radioisotopes. For a synchrotron, one applies a positive ion source in combination with an injector linac. Carbon ion radiotherapy awakens a worldwide interest. About 6000 cancer patients have already been treated with carbon beams from the Heavy Ion Medical Accelerator in Chiba at the National Institute of Radiological Sciences in Japan. These clinical results have clearly verified the advantages of carbon ions. Heidelberg Ion Therapy Center and Gunma University Heavy Ion Medical Center have been successfully launched. Several new facilities are under commissioning or construction. The beam energy is adjusted to the depth of tumors. It is usually between 140 and 430 MeV∕u. Although the beam intensity depends on the irradiation method, it is typically several 10(8) or 10(9) pps. Synchrotrons are only utilized for carbon ion radiotherapy. An ECR ion source supplies multi-charged carbon ions for this requirement. Some other medical applications with ion beams attract developer's interests. For example, the several types of accelerators are under development for the boron neutron capture therapy. This treatment is conventionally demonstrated by a nuclear reactor, but it is strongly expected to replace the reactor by the accelerator. We report status of ion source for medical application and such scope for further developments.
[1]
Y. Iwashita,et al.
Phase rotation scheme of laser-produced ions for reduction of the energy spread
,
2006
.
[2]
R. Iannucci,et al.
Electron cyclotron resonance ion sources in use for heavy ion cancer therapy.
,
2008,
The Review of scientific instruments.
[3]
R. Baartman,et al.
On the development of a 15 mA direct current H− multicusp source
,
1996
.
[4]
W. Beeckman,et al.
Progress Report On the Iba Shi Small Cyclotron for Cancer-therapy
,
1993
.
[5]
A. Villari,et al.
General purpose high-performance electron cyclotron resonance ion source for production of multicharged ions
,
1998
.
[6]
A. G. Drentje,et al.
The compact electron cyclotron resonance ion source KeiGM for the carbon ion therapy facility at Gunma University.
,
2010,
The Review of scientific instruments.
[7]
J M Slater,et al.
The proton treatment center at Loma Linda University Medical Center: rationale for and description of its development.
,
1992,
International journal of radiation oncology, biology, physics.
[8]
Jose R. Alonso,et al.
What will it take for laser driven proton accelerators to be applied to tumor therapy
,
2007
.
[9]
A. G. Drentje,et al.
Experiments With Fundamental Aspects Performed in a Small ECR Ion Source for a New Carbon Therapy Facility
,
2008,
IEEE Transactions on Plasma Science.
[10]
Huaizhou Zhao,et al.
Intense heavy ion beam production from IMP LECR3 and construction progress of a superconducting ECR ion source SECRAL
,
2004
.
[11]
Shinichi Minohara,et al.
Heavy ion synchrotron for medical use —HIMAC project at NIRS-Japan—
,
1992
.