# US 4,393,332 A · Gyrotron transverse energy equalizer

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- Number: US 4,393,332 A
- Document ID: US4393332A
- Status: Granted
- Kind: A
- Application number: 06/184,497
- Filed: 1980-09-05
- Granted: 1983-07-12
- Earliest claimed: 1980-09-05
- Assignees: Varian Associates, Inc.
- Inventors: Robert S. Symons
- Web page: https://patentgrep.com/patent/US4393332A

## CPC

- H01J 25/025: {with an electron stream following a helical path}
- H01J: ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS (spark-gaps H01T; electric arc lamps H05B31/00; particle accelerators H05H)

## Abstract

In a Gyrotron electron tube, oscillating motion perpendicular to the axis of a linear electron beam is produced by a helical component of magnetic field. The length along the beam of the helical field is critically chosen so that electrons at various radii from the axis all acquire equal transverse energy.

## Claims

### Claim 1

A gyrotron electron tube comprising:
means for generating a beam of electrons parallel to an axis; and
periodic means for causing all electrons in said beam to gain approximately the same transverse energy, said periodic means including means for generating a steady field component perpendicular to said axis whose direction rotates about said axis as a periodic function of distance along said axis.

### Claim 2 (depends on 1)

The tube of claim 1 wherein said steady field is a magnetic field.

### Claim 3 (depends on 2)

The tube of claim 2 wherein said periodic means comprises a bifilar helix for conducting counterrotating electric currents.

### Claim 4

A method for operating a gyrotron electron tube comprising means for forming a beam of electrons parallel to an axis, said method comprising the steps of applying a steady periodic field component perpendicular to said axis whose direction rotates about said axis as a periodic function of distance along said axis, and correlating the strength and axial length of said periodic field so that all electrons in said beam at different initial distances from said axis acquire approximately the same transverse energy.

### Claim 5 (depends on 4)

The method of claim 4 wherein said steady field is a magnetic field.

### Claim 6 (depends on 5)

The method of claim 5 wherein said steady field is generated by passing electric current through a bifilar helical conductor outside said beam, said current being of opposite direction in adjacent turns.

### Claim 7

In a gyrotron tube:
means for generating a beam of electrons parallel to an axis; and
means for generating a steady periodic field component perpendicular to said axis whose direction rotates about said axis as a periodic function of distance along said axis and whose strength and axial length are correlated to impart the same transverse energy gain to all electrons in said beam despite differences in initial electron distances from said axis.
