Method and apparatus for synchronizing charged particle pulses with light pulses

Patent metadata

Field	Value
Publication number	US-11715617-B2
Application number	US-202117407748-A
Country	US
Kind code	B2
Filing date	Aug 20, 2021
Priority date	Feb 22, 2019
Publication date	Aug 1, 2023
Grant date	Aug 1, 2023

Abstract

Some embodiments of the present disclosure provide a method that includes colliding a laser with an electron beam to produce backscattered x-rays while the electron beam is traversing a circular arc. This backscattering process is inverse Compton scattering (ICS). ICS x-rays are emitted in the same direction as the electrons. Because this ICS direction is changing as a function of time, the position of the x-ray beam on a detector will change depending on the timing of electron/laser collision. This position change is easily detected and converted to a timing measurement sensitive at the femtosecond scale, converting a very difficult timing measurement of laser pulse, electron pulse, and x-ray pulse synchronization into a simple and robust position measurement.

First claim

What is claimed is:

1. A method, comprising:
directing a first light beam to intersect with a charged particle beam at a first location in a first region to produce a first x-ray beam;
detecting a position on a detector where at least a portion of the first x-ray beam impinges; and
determining a timing synchronization of the charged particle beam relative to the first light beam based on the position.

2. The method of claim 1 , further comprising:
directing a second light beam to intersect the charged particle beam, before the first light beam intersects the charged particle beam, to produce a second x-ray beam; and
directing the second x-ray beam to an experimental end station.

3. The method of claim 2 , wherein the first light beam and the second light beam are derived from a common light source.

4. The method of claim 3 , further comprising directing a third light beam from the common light source to the experimental end station.

5. The method of claim 3 , wherein a larger portion of energy from the common light source is in the second light beam than in the first light beam.

6. The method of claim 1 , wherein the charged particle beam travels along a curved trajectory caused by a magnetic field in the first region.

7. The method of claim 6 , wherein the timing synchronization is a function of a position along the curved trajectory at which the first light beam intersects the charged particle beam.

8. The method of claim 7 , wherein the position on the detector is determined by the position along the curved trajectory at which the first light beam intersects the charged particle beam.

9. The method of claim 6 , further comprising selecting a magnitude of the magnetic field so that charged particles having a central energy in the charged particle beam travel along a selected path.

10. The method of claim 1 , further comprising:
recording a first position on the detector where a first x-ray pulse impinges, the first x-ray pulse generated using a first pulse of the charged particle beam and a first pulse of the first light beam;
recording a second position on the detector where a second x-ray pulse impinges, the second x-ray pulse generated using a second pulse of the charged particle beam and a second pulse of the first light beam; and
converting a distance between the first position and the second position to time delays between respective times of arrival of respective pulses of the charged particle beam relative to respective pulses of the first light beam.

11. The method of claim 10 , wherein converting the distance to the time delay is based on a distance between the first location and the detector.

12. The method of claim 1 , wherein the first x-ray beam is produced through inverse Compton scatter (ICS).

13. The method of claim 1 , wherein the charged particle beam is a relativistic beam.

14. The method of claim 1 , wherein the first light beam is a pulsed laser beam.

15. The method of claim 1 , wherein the charged particle beam comprises an electron beam.

16. The method of claim 15 , wherein the electron beam comprises pulses of electrons.

17. The method of claim 16 , wherein the first light beam comprises pulses of light and a repetition rate of the pulses of light is equal to a repetition rate of the pulses of electrons.

18. The method of claim 17 , wherein the repetition rate is 1 kHz.

19. A time synchronization device, comprising:
a detector configured to measure a position where an x-ray pulse produced by a charged particle beam impinges on the detector;
a camera configured to produce an image of the position on the detector where the x-ray pulse impinges; and
a computer system including one or more processors and memory storing instructions for converting the position on the detector to a measurement of a timing synchronization between the charged particle beam and a light beam.

20. The time synchronization device of claim 19 , wherein the x-ray pulse is produced by colliding the charged particle beam with the light beam from a light source.

21. The time synchronization device of claim 20 , wherein the charged particle beam collides with the light beam in a region having a magnetic field.

22. The time synchronization device of claim 21 , wherein the magnetic field is configured to cause the charged particle beam to travel on a curved trajectory.

23. The time synchronization device of claim 19 , wherein the detector is configured to be placed within a housing that is held under vacuum.

24. The time synchronization device of claim 23 , wherein the camera is configured to be placed outside the housing.

25. The time synchronization device of claim 19 , wherein the detector comprises a scintillator, and the scintillator is configured to emit luminescence when excited by the x-ray pulse.

26. The time synchronization device of claim 25 , wherein the scintillator comprises a yttrium aluminum garnet (YAG) screen.

27. The time synchronization device of claim 19 , wherein the charged particle beam is produced by an accelerator.

28. The time synchronization device of claim 19 , wherein the charged particle beam is a relativistic beam.

29. The time synchronization device of claim 19 , wherein the light beam comprises a pulsed laser beam.

30. The time synchronization device of claim 19 , wherein the charged particle beam comprises an electron beam.

31. The time synchronization device of claim 30 , wherein the electron beam comprises pulses of electrons.

32. The time synchronization device of claim 31 , wherein the light beam comprises pulses of light and a repetition rate of the pulses of light is equal to a repetition rate of the pulses of electrons.

33. The time synchronization device of claim 32 , wherein the repetition rate is 1 kHz.

34. A method, comprising:
determining a timing synchronization between an electron pulse and a light pulse;
generating an x-ray pulse by colliding the light pulse with the electron pulse at a first location;
measuring a position on a detector where the x-ray pulse impinges; and
calculating the timing synchronization based on the position and a distance between the detector and the first location.

35. The method of claim 34 , wherein the first location is within a magnetic field and the electron pulse travels along a circular trajectory.

36. The method of claim 35 , wherein calculating the timing synchronization further comprises using a value of a radius of curvature of the circular trajectory of the electron pulse.

Assignees

• Univ Arizona State

Inventors

• Graves William
• Holl Mark

Classifications

• H04N23/30

  for generating image signals from X-rays · CPC title

• H01J35/153 Primary

  Spot position control · CPC title

• H05G1/02

  Constructional details · CPC title

• H05G1/28

  Measuring or recording actual exposure time; Counting number of exposures; Measuring required exposure time · CPC title

• H05G1/52

  Target size or shape; Direction of electron beam, e.g. in tubes with one anode and more than one cathode · CPC title