Systems and methods for cargo scanning and radiotherapy using a traveling wave linear accelerator based X-ray source using pulse width to modulate pulse-to-pulse dosage
Provided herein are systems and methods for operating a traveling wave linear accelerator to generate stable electron beams at two or more different intensities by varying the number of electrons injected into the accelerator structure during each pulse by varying the width of the beam pulse, i.e., pulse width. The electron beams may be used to generate x-rays having selected doses and energies, which may be used for cargo scanning or radiotherapy applications.
1. A traveling wave linear accelerator for generating a plurality of dose rates and energies of electrons, the traveling wave linear accelerator comprising:
an electron gun modulator configured to adjust a pulse width and a beam injection time of a beam of electrons from an electron gun;
a frequency/power controller configured to determine a frequency and a power of a radio frequency (RF) signal to be generated; and
an intensity controller operatively associated with the electron gun modulator and the frequency/power controller, the intensity controller configured to receive a plurality of intensity/energy adjustment commands and to respectively determine a pulse width, a beam injection time, an RF power factor, and a frequency adjustment factor based on each intensity/energy adjustment command to provide a respective output dose rate and energy of electrons;
wherein, for each intensity/energy adjustment command, the electron gun modulator receives the determined pulse width and the determined beam injection time and adjusts the pulse width and the beam injection time of the beam of electrons and the frequency/power controller receives the frequency adjustment factor and the RF power factor and adjusts the frequency and power of the RF signal such that the traveling wave linear accelerator generates electrons having the respective output dose rate and energy.
2. The traveling wave linear accelerator of claim 1 , further comprising:
an x-ray target configured to generate x-rays responsive to irradiation with electrons, the x-rays irradiating a cargo container; and
a detector configured to detect x-rays transmitted through the container.
3. The traveling wave linear accelerator of claim 2 , further comprising a control unit operatively associated with the detector and with the intensity controller, the control unit being configured:
to send a first intensity/energy adjustment command to cause the intensity controller to determine a first pulse width, a first beam injection time, a first RF power factor and a first frequency adjustment factor to provide a first output dose rate and first energy of a first set of electrons;
to determine a percent transmission of a first set of x-rays through the container based on an output of the detector, the first set of x-rays being generated by the first set of electrons; and
if the percent transmission is below a predetermined threshold, to send a second intensity/energy adjustment command to cause the intensity controller to determine a second pulse width, a second beam injection time, a second RF power factor, and a second frequency adjustment factor to provide a second output dose rate and second energy of a second set of electrons.
4. The traveling wave linear accelerator of claim 3 , wherein the second energy is higher than the first energy.
5. The traveling wave linear accelerator of claim 4 , wherein the intensity controller is configured to select the second output dose rate of the second set of electrons such that a dose of the first set of x-rays is about the same as a dose of a second set of x-rays generated by the second set of electrons.
6. The traveling wave linear accelerator of claim 3 , wherein the control unit is configured:
to determine a percent transmission of a second set of x-rays through the container based on an output of the detector, the second set of x-rays being generated by the second set of electrons; and
if the percent transmission is below a predetermined threshold, to send a third intensity/energy adjustment command to cause the intensity controller to determine a third pulse width, a third beam injection time, a third RF power factor, and a third frequency adjustment factor to provide a third output dose rate and third energy of a third set of electrons.
7. The traveling wave linear accelerator of claim 6 , wherein the third energy is higher than the second energy.
8. The traveling wave linear accelerator of claim 7 , wherein the intensity controller is configured to select the third output dose rate of the third set of electrons such that a dose of the second set of x-rays is about the same as a dose of a third set of x-rays generated by the third set of electrons.
9. The traveling wave linear accelerator of claim 6 , wherein the third energy is lower than the second energy and wherein the intensity controller is configured to select the third output dose rate of the third set of electrons such that a dose of a third set of set x-rays is greater than a dose of the first set of x-rays generated by the first set of electrons.
10. The traveling wave linear accelerator of claim 2 , further comprising a control unit operatively associated with the detector and with the intensity controller, the control unit being configured:
to send a first intensity/energy adjustment command to cause the intensity controller to determine a first pulse width, a first beam injection time, a first RF power factor, and a first frequency adjustment factor to provide a first output dose rate and first energy of a first set of electrons;
to determine a percent transmission of a first set of x-rays through the container based on an output of the detector, the first set of x-rays being generated by the first set of electrons; and
if the percent transmission is above a predetermined threshold, to send a second intensity/energy adjustment command to cause the intensity controller to determine a second pulse width, a second beam injection time, a second RF power factor, and a second frequency adjustment factor to provide a second output dose rate and a second energy of a second set of electrons.
11. The traveling wave linear accelerator of claim 10 , wherein the intensity controller is configured to select the second output dose rate of the second set of electrons such that a dose of a second set of x-rays generated by the second set of electrons is less than a dose of the first set of x-rays.
12. The traveling wave linear accelerator of claim 1 , further comprising:
an x-ray target configured to generate x-rays responsive to irradiation with electrons from the traveling wave linear accelerator, the x-rays being configured to irradiate a tumor volume; and
a robotic arm on which the x-ray target and the linear accelerator are mounted and configured to adjust an angle at which the x-rays irradiate the tumor volume.
13. The traveling wave linear accelerator of claim 12 , further comprising a control unit operatively associated with the robotic arm and with the intensity controller, the control unit being configured:
to send a first intensity/energy adjustment command to cause the intensity controller to determine a first pulse width, a first beam injection time, a first RF power factor, and a first frequency adjustment factor to provide a first output dose rate and a first energy of a first set of electrons;
to send a first position command to the robotic arm to cause the robotic arm to adjust the angle to irradiate a first portion of the tumor volume with x-rays generated by the first set of electrons;
to send a second intensity/energy adjustment command to cause the intensity controller to determine a second pulse width, a second beam injection time, a second RF power factor, and a second frequency adjustment factor to provide a second output dose rate and a second energy of a second set of electrons; and
to send a second position command to the robotic arm to cause the robotic arm to adjust the angle to irradiate a second portion of the tumor volume with x-rays generated by the second set of electrons.
14. The traveling wave linear accelerator of claim 13 , wherein the second energy is higher than the first energy.
15. The traveling wave linear accelerator of claim 14 , wherein the second tumor volume is deeper than the first tumor volume.
16. The traveling wave linear accelerator of claim 13 , wherein the first tumor volume and the second tumor volume receive about the same doses of x-rays as one another.
17. The traveling wave linear accelerator of claim 1 , wherein the frequency/power controller is further configured to determine a pulse risetime of the RF signal to be generated, wherein the intensity controller is further configured to determine a pulse risetime factor based on each intensity/energy adjustment command, and wherein the frequency/power controller is further configured to receive the pulse risetime factor from the intensity controller and to adjust the pulse risetime of the RF signal.
18. A method for generating a plurality of dose rates and energies of electrons using a traveling wave linear accelerator, the traveling wave linear accelerator comprising an electron gun modulator configured to adjust a pulse width and a beam injection time of a beam of electrons from an electron gun and a frequency/power controller configured to adjust a frequency and a power of a radio frequency (RF) signal to be generated, the method comprising:
receiving at an intensity controller a plurality of intensity/energy adjustment commands and respectively determining a pulse width, a beam injection time, an RF power factor, and a frequency adjustment factor based on each intensity/energy adjustment command to provide a respective dose rate and energy of electrons; and for each intensity/energy adjustment command:
adjusting the pulse width and beam injection time of electrons from the electron gun at the electron gun modulator using the determined pulse width and the determined beam injection time;
determining the frequency and power of the RF signal to be generated at the frequency/power controller based on the RF power factor and the frequency adjustment factor; and
generating electrons having the respective output dose rate and energy using the traveling wave linear accelerator.
19. The method of claim 18 , further comprising:
sending a first intensity/energy adjustment command to cause the intensity controller to determine a first pulse width, a first RF power factor and a first frequency adjustment factor to provide a first output dose rate and first energy of a first set of electrons;
generating x-rays with the first set of electrons;
irradiating a cargo container with the x-rays;
determining a percent transmission of a first set of x-rays through the container based on an output of the detector; and
if the percent transmission is below a predetermined threshold, sending a second intensity/energy adjustment command to cause the intensity controller to determine a second pulse width, a second beam injection time, a second RF power factor, and a second frequency adjustment factor to provide a second output dose rate and second energy of a second set of electrons.
20. The method of claim 18 , further comprising:
sending a first intensity/energy adjustment command to cause the intensity controller to determine a first pulse width, a first beam injection time, a first RF power factor, and a first frequency adjustment factor to provide a first output dose rate and a first energy of a first set of electrons;
sending a first position command to a robotic arm on which the linear accelerator and an x-ray target are mounted to cause the robotic arm to adjust an angle to irradiate a first portion of a tumor volume with x-rays generated by the first set of electrons;
sending a second intensity/energy adjustment command to cause the intensity controller to determine a second pulse width, a second beam injection time, a second RF power factor, and a second frequency adjustment factor to provide a second output dose rate and a second energy of a second set of electrons; and
sending a second position command to the robotic arm to cause the robotic arm to adjust the angle to irradiate a second portion of the tumor volume with x-rays generated by the second set of electrons.
21. The method of claim 18 , further comprising determining at the intensity controller a pulse risetime factor based on each intensity/energy adjustment command, and adjusting a pulse risetime of the RF signal based on the pulse risetime factor.