IP Library › Granted Patent US 11,013,100
Granted Patent B2
US 11,013,100 · App. 16/341,039 · Granted May 18, 2021

Plasma accelerator

Inventors: Bernhard Hidding (Glasgow, GB); Grace Manahan (Glasgow, GB); Fahim Ahmad Habib (Glasgow, GB); Paul Scherkl (Glasgow, GB)
Assignee: University of Strathclyde
H05H1/54H01S3/0903H05H1/46H05H15/00
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Quick Facts
Patent No.
US 11,013,100
App. No.
16/341,039
Granted
May 18, 2021
Kind
B2
Abstract

A method of accelerating charged particles in a plasma and an associated plasma accelerator and electromagnetic radiation source, the method including creating a region of non-uniform electric field within the plasma which propagates through the plasma; using the non-uniform electric field to accelerate a first plurality of charged particles in the direction of propagation of the region of non-uniform electric field; and once the accelerating first plurality of charged particles have propagated part-way through the plasma: adding a second plurality of charged particles to the plasma, such that the second plurality of charged particles propagates through the plasma, the second plurality of charged particles create a local distortion in the non-uniform electric field experienced by the accelerating first plurality of charged particles, and the local distortion in the non-uniform electric field propagates through the plasma with the accelerating first plurality of charged particles; and the method also including using the local distortion in the non-uniform electric field to accelerate the first plurality of charged particles in the direction of propagation of the region of non-uniform electric field.

Claims (35)

1. A method of accelerating charged particles in a plasma, the method comprising the steps of:

creating a region of non-uniform electric field within the plasma which propagates through the plasma;

using the non-uniform electric field to accelerate a first plurality of charged particles in the direction of propagation of the region of non-uniform electric field;

once the accelerating first plurality of charged particles have propagated part-way through the plasma:

(A) adding a second plurality of charged particles to the plasma, such that:

(i) the second plurality of charged particles propagates through the plasma with the accelerating first plurality of charged particles,

(ii) the second plurality of charged particles creates a local distortion in the non-uniform electric field experienced by the accelerating first plurality of charged particles, and

(iii) the local distortion in the non-uniform electric field propagates through the plasma with the accelerating first plurality of charged particles; and

(B) using the local distortion in the non-uniform electric field to accelerate the first plurality of charged particles in the direction of propagation of the region of non-uniform electric field.

2. The method of claim 1 , wherein the energy distribution of the first plurality of charged particles broadened due to the non-uniform electric field, and the energy distribution of the first plurality of charged particles is at least partially narrowed due to the local distortion in the non-uniform electric field.

3. The method of claim 1 , wherein the energy distribution of the first plurality of charged particles due to the non-uniform electric field and due to the local distortion in the electric field is equal or within a threshold amount.

4. The method of claim 1 , wherein at least one of the first or the second plurality of charged particles comprise a group, bunch, collection, packet, or beam of charged particles.

5. The method of claim 1 , wherein at least one of the first or the second plurality of charged particles comprise at least one of electrons, positrons, protons, or ions.

6. The method of claim 1 , wherein the non-uniform electric field is created by the propagation of a plasma wave through the plasma.

7. The method of claim 6 , wherein the plasma wave is created by a laser beam or particle beam interacting with the plasma.

8. The method of claim 1 , wherein the plasma comprises a low ionization threshold component and a high ionization threshold component.

9. The method of claim 8 , wherein the plasma wave propagates in the low ionization threshold component.

10. The method of claim 1 , wherein the first plurality of charged particles are created by the under-dense photocathode Trojan Horse method.

11. The method of claim 8 , wherein the second plurality of charged particles are electrons ionized from the high ionization threshold component.

12. A plasma accelerator configured to implement the method of claim 1 , the plasma accelerator comprising:

a plasma generator;

a first excitation source configured to create the non-uniform electric field which propagates through the plasma and which accelerates the first plurality of charged particles in the direction of propagation of the region of non-uniform electric field or, is configured to create the first plurality of charged particles within the plasma;

a second excitation source configured to create the second plurality of charged particles within the plasma once the first plurality of charged particles have propagated part-way through the plasma, wherein the second plurality of charged particles propagate through the plasma with the accelerating first plurality of charged particles, create the local distortion in the non-uniform electric field experienced by the accelerating first plurality of charged particles, the local distortion in the non-uniform electric field configured to accelerate the first plurality of charged particles in the direction of propagation of the region of non-uniform electric field; and

an external controller configured to control when at least one of the first or the second excitation sources interact with the plasma.

13. The plasma accelerator of claim 12 , wherein at least one of the first or the second excitation sources comprise at least one laser.

14. The plasma accelerator of claim 12 , wherein the plasma generator comprises a heater or an electromagnetic field generator.

15. The plasma accelerator of claim 12 , comprising at least one of:

a first transport system, configured to transport at least one of the first plurality of charged particles or the first excitation source into the plasma; or

a second transport system, configured to collect the first plurality of charged particles from the plasma.

16. An electromagnetic radiation source comprising the plasma accelerator of claim 12 .

17. The electromagnetic radiation source of claim 16 , wherein the electromagnetic radiation source is one of:

a free-electron laser,

an inverse Compton scattering light source, or

an ion channel laser.

18. The electromagnetic radiation source of claim 17 , wherein the inverse Compton scattering light source or the ion channel laser operate within the plasma of the plasma accelerator.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Nov 16, 2020
From: SCHERKL, PAUL
To: UNIVERSITY OF STRATHCLYDE
Reel/Frame 054375/0775 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Apr 26, 2019
From: HIDDING, BERNHARD; MANAHAN, GRACE; HABIB, FAHIM AHMAD
To: UNIVERSITY OF STRATHCLYDE
Reel/Frame 049014/0184 →
Priority Claims (1)
GB 1617173 · Oct 10, 2016 · national
Continuity (1)
Related Publication 20190239332A1 · Aug 1, 2019