IP Library Granted Patent US 9,673,015
Granted Patent B2
US 9,673,015 · App. 14/846,151 · Granted Jun 6, 2017

Partially grounded depressed collector

Inventors: Yong Jiang (New Haven, CT); Vladimir Teryaev (Protvino, RU); Jay Hirshfield (Orange, CT)
Assignees: OMEGA-P, INC.; YALE UNIVERSITY
H01J23/027H01J23/0275H01J25/10
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Quick Facts
Patent No.
US 9,673,015
App. No.
14/846,151
Granted
Jun 6, 2017
Kind
B2
Abstract

A depressed beam collector and an RF source comprising a depressed beam collector. The RF source may include, e.g., a multi-beam klystron, a single beam klystron, or other RF sources having an electron gun. The beam collector collects spent electrons from the electron gun and comprises a grounded portion configured to collect a portion of electrons entering the collector and a biased portion configured to collect another portion of the electrons entering the collector and having a depressed energy.

Claims (39)

1. A depressed beam collector comprising:

a grounded portion configured to collect a portion of electrons entering the collector;

a biased portion configured to collect another portion of the electrons entering the collector and having a depressed energy, wherein the grounded portion and the biased portion each form a portion of a wall of the depressed beam collector;

a high voltage gap comprising a spacing in the wall between the grounded portion and the biased portion; and

a magnetic lens at least partially surrounding the high voltage gap.

2. The depressed beam collector of claim 1 , wherein the beam collector comprises a plurality of channels, each channel corresponding to one of a plurality of electron beams.

3. The depressed beam collector of claim 1 , wherein the biased portion is coupled to a depressed power supply at a collector voltage.

4. The depressed beam collector of claim 1 , wherein the magnetic lens is configured to suppress reflection of a spent beam functioning in concert with the space charge distribution.

5. The depressed beam collector of claim 4 , wherein the magnetic lens is configured to create a magnetic field for guiding a spent beam to penetrate the grounded portion and then to disperse.

6. The depressed beam collector of claim 5 , wherein the magnetic field is configured to disperse the spent beam near and beyond a high voltage gap.

7. The depressed beam collector of claim 1 ,

wherein the magnetic lens comprises an iron pole piece at least partially surrounding the high voltage gap.

8. The depressed beam collector of claim 1 , wherein the depressed beam collector comprises space charge forces configured to disperse a trajectory of a decelerated spent beam.

9. The depressed beam collector of claim 1 , wherein the beam collector is a single-stage depressed beam collector.

10. The depressed beam collector of claim 1 , wherein the beam collector is a multi-stage depressed beam collector.

11. The depressed beam collector of claim 1 , further comprising cooling channels comprised in the grounded portion and the biased portion.

12. The depressed beam collector of claim 1 , wherein the depressed beam collector comprises a material having a low secondary emission coefficient.

13. The depressed beam collector of claim 1 , further comprising:

a coating of a material having a low secondary emission coefficient.

14. An RF source comprising:

an electron gun; and

a depressed beam collector including:

a grounded portion configured to collect a portion of electrons entering the collector;

a biased portion configured to collect another portion of the electrons entering the collector and having a depressed energy, wherein the grounded portion and the biased portion each form a portion of a wall of the depressed beam collector;

a high voltage gap comprising a spacing in the wall between the grounded portion and the biased portion; and

a magnetic lens at least partially surrounding the high voltage gap.

15. The RF source of claim 14 , wherein the electron gun is configured to emit a plurality of electron beams, and wherein the beam collector comprises a plurality of channels, each channel corresponding to one of the plurality of electron beams.

16. The RF source of claim 14 , wherein the biased portion is coupled to a depressed power supply at a collector voltage.

17. The RF source of claim 14 , wherein the magnetic lens is configured to suppress reflection of a spent beam.

18. The RF source of claim 14 , wherein the

magnetic lens comprises an iron pole piece at least partially surrounding the high voltage gap.

19. An RF source comprising:

a multi-beam klystron; and

a depressed beam collector including:

a grounded portion configured to collect a portion of electrons entering the collector;

a biased portion configured to collect another portion of the electrons entering the collector and having a depressed energy, wherein the grounded portion and the biased portion each form a portion of a wall of the depressed beam collector;

a high voltage gap comprising a spacing in the wall between the grounded portion and the biased portion; and

a magnetic lens at least partially surrounding the high voltage gap.

20. The RF source of claim 19 , wherein the biased portion is coupled to a depressed power supply at a collector voltage.

Assignments (3)
CONFIRMATORY LICENSE Recorded Sep 26, 2017
From: OMEGA-P, INC.
To: UNITED STATES DEPARTMENT OF ENERGY
Reel/Frame 043704/0689 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 23, 2015
From: TERYAEV, VLADIMIR
To: OMEGA-P, INC.
Reel/Frame 036871/0346 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 23, 2015
From: JIANG, YONG; HIRSHFIELD, JAY
To: YALE UNIVERSITY
Reel/Frame 036871/0366 →
Continuity (2)
Provisional Application 62046053 · Sep 4, 2014
Related Publication 20160071681A1 · Mar 10, 2016