DETERMINATION OF HEAVY PARTICLE STOPPING POWER

• US 20090274269A1
• Filed: 05/01/2009
• Published: 11/05/2009
• Est. Priority Date: 05/02/2008
• Status: Active Grant

• Current Assignee: L-3 Communications Security & Detection Systems, Inc. (Leidos Holdings, Inc.)
• Original Assignee: L-3 Communications Security & Detection Systems, Inc. (Leidos Holdings, Inc.)
• Inventors: Oreper, Boris, Foland, Andrew Dean
• Granted Patent: US 7,903,781 B2
• Time in Patent Office: Days
• US Class Current: 378/54
• CPC Class Codes: A61N 2005/1061 using an x-ray imaging system having a separate imaging source
• CPC Class Codes: A61N 2005/1087 Ions; Protons
• CPC Class Codes: A61N 5/1048 Monitoring, verifying, controlling systems and methods

Abstract

A distribution of heavy particle stopping power is be determined. A distribution of effective atomic number of a three-dimensional space is accessed, and a distribution of an x-ray stopping power of the three-dimensional space is accessed. A conversion is applied to the distribution of the effective atomic number and the distribution of x-ray stopping power. A distribution of the heavy particle stopping power of the three-dimensional space is generated based on the conversion, the heavy particle stopping power being an indication of a depth of penetration for a heavy particle incident on the three-dimensional space.

Claims

1. A system for determining a distribution of heavy particle stopping power of a patient, the system comprising:

a broadband source of dual-energy x-rays, the broadband source configured to;

produce a beam of broadband x-ray radiation, the broadband beam including energy having a first energy spectrum and a first peak energy and energy having a second energy spectrum and a second peak energy, and

irradiate a three-dimensional space within a patient with the beam of broadband x-ray radiation;

a detector system comprising a sensor configured to;

sense radiation from the three-dimensional space, the sensed radiation including radiation caused by irradiating the three-dimensional space with the broadband source, and

produce a representation of the sensed radiation; and

a processor operable to;

receive the representation of the sensed radiation,

determine a distribution of effective atomic number of the three-dimensional space based on the representation from the detector system,

determine a distribution of an x-ray stopping power of the three-dimensional space based on the representation from the detector system, the x-ray stopping power of the three-dimensional space being an indication of a depth of penetration of an x-ray incident on the three-dimensional space,

apply a conversion to the distribution of the x-ray stopping power and the distribution of the effective atomic number, and

generate a distribution of a heavy particle stopping power of the three-dimensional space based on the conversion, the heavy particle stopping power being used to indicate a depth of penetration for a heavy particle incident on the three-dimensional space.

2. The system of claim 1, wherein the processor is further operable to produce an input sufficient to define a heavy particle treatment based on the heavy particle stopping power, the input including a depth of penetration for a particular heavy particle.

3. The system of claim 1, further comprising a heavy particle therapy system comprising:

a source of heavy particles configured to;

produce a beam including a heavy particle, and

direct the beam to a position within the three-dimensional space; and

an input module configured to receive the distribution of the heavy particle stopping power of the three-dimensional space from the processor.

4. The system of claim 3, wherein the heavy particle therapy system and the broadband source of dual-energy x-rays are co-located.

5. The system of claim 4, wherein the heavy particle therapy system and the broadband source of dual-energy x-rays are located on a gantry.

6. The system of claim 1, further comprising a gantry on which the broadband source of dual-energy x-rays and the detector system are mounted.

7. The system of claim 1, wherein the broadband source of dual-energy x-rays comprises a single broadband source that is switchable between a first mode and a second mode, the single broadband source producing a first x-ray beam in the first mode and a second x-ray beam in the second mode, the first x-ray beam having the first energy spectrum and the first peak energy, and the second x-ray beam having the second energy spectrum and the second peak energy.

8. The system of claim 1, wherein the broadband source of dual-energy x-rays comprises:

a first broadband source configured to produce a first x-ray beam having the first energy spectrum and the first peak energy, and

a second broadband source separate from the first broadband source and configured to produce a second x-ray beam having the second energy spectrum and the second peak energy.

9. The system of claim 1, wherein the detector system further comprises a detector configured to detect photons.

10. The system of claim 1, wherein the detector system is positioned opposite the three-dimensional space relative to the broadband source.

11. A system for determining a distribution of heavy particle stopping power of a patient, the system comprising:

a broadband source of x-rays configured to;

produce a single beam of broadband x-ray radiation having an energy spectrum and a peak energy, and

irradiate a three-dimensional space within a patient with the beam of broadband x-ray radiation;

a dual-energy detector system comprising a first sensor including a first sensor relatively more sensitive to a first band of energies included in the broadband x-ray radiation, and a second sensor relatively more sensitive to a second band of energies included in the broadband x-ray radiation, the second band of energies being higher than the first band of energies, and the sensor being configured to;

sense radiation from the three-dimensional space, the sensed radiation including radiation caused by irradiating the three-dimensional space with the broadband source, and

produce a representation of the sensed radiation; and

a processor operable to;

receive the representation of the sensed radiation,

determine a distribution of effective atomic number of the three-dimensional space based on the representation from the detector system,

determine a distribution of an x-ray stopping power of the three-dimensional space based on the representation from the detector system, the x-ray stopping power of the three-dimensional space being an indication of a depth of penetration of an x-ray incident on the three-dimensional space,

apply a conversion to the distribution of the x-ray stopping power and the distribution of the effective atomic number, and

generate a distribution of a heavy particle stopping power of the three-dimensional space based on the conversion, the heavy particle stopping power being used to indicate a depth of penetration for a heavy particle incident on the three-dimensional space.

12. A computer-readable storage medium storing instructions, that when executed, cause a processor to perform the following operations:

access data reflecting an interaction between a broadband x-ray beam and a three-dimensional space of a patient, the broadband x-ray beam including a first energy band having a first energy spectrum and a first peak energy, and a second energy band having a second energy spectrum and a second peak energy higher than the first peak energy;

analyze the accessed data to determine an interaction between the three-dimensional space and the first energy band and an interaction between the three-dimensional space and the second energy band;

determine a distribution of effective atomic number of a three-dimensional space based on the interactions between the three-dimensional space and the first and second energy bands;

access a distribution of x-ray stopping power of the three-dimensional space;

apply a conversion to the distribution of the effective atomic number and the distribution of the x-ray stopping power of the three-dimensional space; and

generate, based on the conversion, a heavy particle distribution that represents a heavy particle stopping power of the three-dimensional space, the heavy particle stopping power being used to indicate a depth of penetration for a heavy particle incident on the three-dimensional space.

13. The medium of claim 12, wherein the instructions further comprise instructions, that when executed, cause the processor to provide inputs sufficient to define a heavy particle treatment that is directed toward a particular space within the three-dimensional space, the inputs being derived from the heavy particle distribution and the inputs including a depth of penetration for a particular heavy particle.

14. The medium of claim 13, wherein the inputs include a three-dimensional location of a target space within a body of a patient.

15. The medium of claim 13, wherein the particular heavy particle is one of a proton, a heavy ion, or a pion.

16. The medium of claim 12, wherein the first energy spectrum and the second energy spectrum overlap.

17. The medium of claim 12, wherein the three-dimensional space is represented by one or more voxels, and the distribution of the effective atomic number includes an effective atomic number for each voxel.

18. The medium of claim 12, wherein the heavy particle distribution is a volumetric heavy particle stopping power distribution.

19. The medium of claim 12, wherein the heavy particle distribution is a two-dimensional stopping power distribution.

20. A computer-readable storage medium storing instructions, that when executed, cause a processor to perform the following operations:

access a distribution of effective atomic number of a three-dimensional space;

access a distribution of an x-ray stopping power of the three-dimensional space;

apply a conversion to the distribution of the effective atomic number and the distribution of x-ray stopping power; and

generate a distribution of the heavy particle stopping power of the three-dimensional space based on the conversion, the heavy particle stopping power being an indication of a depth of penetration for a heavy particle incident on the three-dimensional space.

21. The medium of claim 20, wherein the distribution of the heavy particle stopping power distribution is a volumetric distribution.

22. The medium of claim 20, wherein the distribution of the heavy particle stopping power distribution is a two-dimensional distribution.

23. A method for determining a distribution of heavy particle stopping power, the method comprising:

accessing a distribution of effective atomic number of a three-dimensional space;

accessing a distribution of an x-ray stopping power of the three-dimensional space;

applying a conversion to the distribution of the effective atomic number and the distribution of x-ray stopping power; and

generating a distribution of the heavy particle stopping power of the three-dimensional space based on the conversion, the heavy particle stopping power being an indication of a depth of penetration for a heavy particle incident on the three-dimensional space.