Synchrotron power supply apparatus and method of use thereof
View Patent ↗The invention comprises a charged particle cancer therapy system or synchrotron system using a single power supply electrically connected to a plurality of magnet sections to provide a uniform current to a plurality of magnets at a given period in time. Optionally, one or more switches introduce a corresponding one or more resistors into a circuit linking the power supply to a magnet or an inductor during an applied power recovery phase between acceleration cycles of the synchrotron, which reduces time of reduction in power from an active applied power to a power suitable for use with a subsequent injection of charged particles into the synchrotron.
1. An apparatus for cancer therapy using charged particles, comprising:
a synchrotron, said synchrotron comprising:
a set of n bending magnets configured to turn the charged particles in a circulation beam path during an acceleration phase of said synchrotron, wherein n is a positive integer of at least four; and
a single power supply simultaneously electrically linked to all of said n bending magnets;
a center, wherein the charged particle circulation beam path passes;
about said center;
through straight sections; and
through turning sections,
at least one inductor wrapped about a portion of each turning section; and
an electric circuit configured to link said power supply to said inductor, said power supply configured to deliver a first voltage at a terminus of the acceleration phase to said inductor about said synchrotron,
wherein said electric circuit comprises:
at least one electric switch alternately configurable in an open position and in a closed position; and
at least one resistor, said switch configured in said open position to direct current through said resistor during a recovery period following the terminus of the acceleration phase,
wherein each of said turning sections comprises a plurality of said bending magnets, and
wherein a number of said straight sections equals a number of said turning sections.
2. The apparatus of claim 1 , wherein said set of n bending magnets comprises an even number of at least sixteen bending magnets.
3. An apparatus for cancer therapy using charged particles, comprising:
a synchrotron, said synchrotron comprising:
a set of n bending magnets configured to turn the charged particles in a circulation beam path during an acceleration phase of said synchrotron, wherein n is a positive integer of at least four; and
a single power supply simultaneously electrically linked to all of said n bending magnets,
wherein at least two of said bending magnets further comprise a magnetic field focusing section, said focusing section comprising:
a magnet core geometry tapering as a continuous function from a first cross-sectional area to a parallel second cross-sectional area, said second cross-sectional area comprising less than two-thirds of an area of said first cross-sectional area, said second cross-sectional area proximate the circulation beam path.
4. An apparatus for cancer therapy using charged particles, comprising:
a synchrotron, said synchrotron comprising:
a set of n bending magnets configured to turn the charged particles in a circulation beam path during an acceleration phase of said synchrotron, wherein n is a positive integer of at least four;
a single power supply simultaneously electrically linked to all of said n bending magnets;
a center, wherein the charged particle circulation beam path passes;
about said center;
through straight sections; and
through turning sections, and
a first focusing edge; a second focusing edge; a third focusing edge; and a fourth focusing edge,
wherein each of said turning sections comprises a plurality of said bending magnets,
wherein a number of said straight sections equals a number of said turning sections,
wherein a first of said turning sections comprises a first bending magnet and a second bending magnet of said n bending magnets,
wherein said first bending magnet terminates on opposite sides with said first focusing edge and said second focusing edge,
wherein a first plane established by said first focusing edge intersects a second plane established by said second focusing edge beyond said center of said synchrotron,
wherein said second bending magnet terminates on opposite sides with said third focusing edge and said fourth focusing edge,
wherein a third plane established by said third focusing edge intersects a fourth plane established by said fourth focusing edge beyond said center of said synchrotron, and
wherein all of said first focusing edge; said second focusing edge; said third focusing edge; and said fourth focusing edge bend the charged particles toward said center of said synchrotron during use.
5. An apparatus for cancer therapy using charged particles, comprising:
a synchrotron, said synchrotron comprising:
a set of n bending magnets configured to turn the charged particles in a circulation beam path during an acceleration phase of said synchrotron, wherein n is a positive integer of at least four; and
a single power supply simultaneously electrically linked to all of said n bending magnets, and
a center,
wherein the charged particle circulation beam path passes;
about said center;
through straight sections; and
through turning sections,
wherein each of said turning sections comprises a plurality of said bending magnets,
wherein a number of said straight sections equals a number of said turning sections, and
wherein said turning sections each comprise at least four of said n bending magnets, said at least four of said n bending magnets comprising at least eight edge focusing surfaces, said geometry of said edge focusing surfaces configured to focus the charged particles in the charged particle circulation beam path during use.
6. The apparatus of claim 1 , wherein during use each of said turning sections turns the charged particles by about ninety degrees.
7. The apparatus of claim 1 , wherein said turning sections comprise exactly four turning sections, wherein during use each of said four turning sections turns the charged particle circulation beam path about ninety degrees, said synchrotron capable of accelerating the charged particles to at least 300 MeV.
8. An apparatus for cancer therapy using charged particles, comprising:
a synchrotron, said synchrotron comprising:
a set of n bending magnets configured to turn the charged particles in a circulation beam path during an acceleration phase of said synchrotron, wherein n is a positive integer of at least four;
a single power supply simultaneously electrically linked to all of said n bending magnets; and
a center,
wherein the charged particle circulation beam path passes;
about said center;
through straight sections; and
through turning sections,
wherein each of said turning sections comprises a plurality of said bending magnets,
wherein a number of said straight sections equals a number of said turning sections, and
wherein said turning sections comprise:
exactly four turning sections; and
at least thirty-two charged particle edge focusing surfaces.
9. The apparatus of claim 1 , said synchrotron further comprising:
a Lamberson magnet, said single power supply linked to said n bending magnets simultaneously linked to said Lamberson magnet.
10. The apparatus of claim 1 , further comprising:
a beam transport path outside of said synchrotron, said beam transport path comprising:
an extraction focusing magnet; and
an extraction turning magnet,
said single power supply linked to said n bending magnets simultaneously electrically linked to said extraction focusing magnet and said extraction turning magnet.
11. The apparatus of claim 1 , wherein said at least one electric switch comprises: a first electric switch and a second electric switch, wherein said at least one resistor comprises a first resistor and a second resistor, said first electric switch configured to switch on and off current through said first resistor, said second electric switch configured to switch on and off current through said second resistor, wherein said first resistor comprises a resistance in a range of one-tenth to four-tenths of an Ohm, wherein said second resistor comprises a resistance greater than four-tenths of an Ohm.
12. The apparatus of claim 1 , wherein said charged particle circulation beam path does not pass through any operational quadrupole magnets.
13. A method for accelerating charged particles for cancer therapy, comprising the steps of:
providing a synchrotron, said synchrotron comprising:
a set of n bending magnets, wherein n is a positive integer of at least four; and
a circulation beam path;
simultaneously providing power from a single power supply to all of said n bending magnets;
turning the charged particles in said circulation beam path during an acceleration phase of said synchrotron using magnetic fields in said bending magnets;
applying a first acceleration voltage, using said single power supply, to an inductor via an electrical circuit during an acceleration period of said synchrotron, said inductor configured to generate a magnetic field through a portion of at least one of said n bending magnets; and
opening a first switch in said electrical circuit to add a first resistor to said electrical circuit during a recovery time period after said acceleration period, wherein said first resistor results in a decrease of said voltage to said inductor.
14. The method of claim 13 , further comprising the step of:
opening a second switch in said electrical circuit to add a second resistor to said electrical circuit during a recovery time period after said step of opening said first switch, wherein said second resistor results in a decrease of said voltage to said inductor.
15. The method of claim 13 , further comprising the step of:
accelerating the charged particles in the circulation beam path, said circulation beam path comprising:
a center;
straight sections; and
turning sections,
wherein said turning sections each comprise at least four bending magnets of said n bending magnets, said four bending magnets comprising at least eight surfaces having focusing geometry, and
wherein a number of said straight sections equals a number of said turning sections.
16. The method of claim 13 , further comprising the steps of:
transmitting the charged particles through an extraction material, said extraction material yielding a reduced energy charged particle beam;
applying at least five hundred volts across a first pair of blades; and
passing the reduced energy charged particle beam between said first pair of blades,
wherein said first pair of blades redirect the reduced energy charged particle beam to a deflector,
wherein said deflector yields an extracted charged particle beam.
17. The method of claim 16 , wherein said extraction material comprises a foil of about forty to sixty microns thickness,
wherein said extraction material comprises atoms, said atoms consisting essentially of atoms having six or fewer protons.
18. The method of claim 13 , further comprising the steps of:
providing a Lamberson magnet in said synchrotron;
providing an extraction focusing magnet in a beam transport path outside of said synchrotron; and
providing an extraction turning magnet in the beam transport path outside of said synchrotron,
said single power supply providing power to said n bending magnets simultaneously providing power to all of: said Lamberson magnet, said extraction focusing magnet, and said extraction turning magnet.