US4570103A
Expired / Lapsed
US
⏱️ 0.0 years remaining
Particle beam accelerators
Assignee: Individual
•
Filing: 1982-09-30
•
Granted: 1986-02-11
•
Expires: 2002-09-30
Abstract
Abstract A technique for accelerating charged particles using an intense traveling electromagnetic wave such as produced by appropriate wavelength lasers. Low energy electrons injected into the focal region of an intense, polarized laser beam are rapidly accelerated in the direction of the beam by the ponderomotive force of the radiation field. The particles reach maximum energy in a distance comparable to the Rayleigh range of a tightly focussed, visible wavelength, diffraction limited pulsed laser. At this point, a combination of induced transverse velocity drifts and/or the rapidly decreasing electric field strengths due to the expanding laser beam envelope cause the particles to enter a low radiation field region before significant deceleration can occur. The resulting device possesses unique advantages and properties not present in existing accelerators.
Inventors
- 👤 Neil C. Schoen
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-11-03 16:10
CPC Classifications
H; H05; H05H; H05H9/00; G; G21; G21K; G21K1/00; H01; H01J; H01J23/00; H01J23/02; H01J23/06; A; A61; A61N; A61N5/00; A61N5/10; A61N2005/1085; A61N2005/1087; A61N2005/1088
Claims Analysis
Total Claims: 10
Claim 1
Independent Claim
175 words
An apparatus for the acceleration of charged particles comprising a source radiation beam of intense coherent polarized traveling electromagnetic waves, means bringing said radiation beams or waves to a near-diffraction limited focal region, with said near-diffraction limited focal region created by an optical or quasi-optical radiation resonator operating in a TEM mode, whereupon a charged particle stream or streams caused to be present at said focal region is accelerated to high energies by the electric field vector of said traveling wave, which is transverse to the direction of propagation of said radiation beam, thereby causing said charged particles to achieve significant transverse velocity, causing them to then interact with the magnetic field vector of said radiation beam via a v×B ponderomotive force, thereby deflecting said charged particles in the direction of said propagating radiation beam and causing the transverse velocity vectors of said charged particles to remain in near synchronism with the electric field vector of said traveling wave and thereby continue to gain energy until said charged particles leave said high field focal region.
Claim 2
Independent Claim
175 words
An apparatus for the acceleration of charged particles comprising a source radiation beam of intense coherent polarized traveling electromagnetic waves, means bringing said radiation beams or waves to a near-diffraction limited focal region, with said near-diffraction limited focal region created by an optical or quasi-optical radiation resonator operating in a TEM mode, whereupon a charged particle stream or streams caused to be present at said focal region is accelerated to high energies by the electric field vector of said traveling wave, which is transverse to the direction of propagation of said radiation beam, thereby causing said charged particles to achieve significant transverse velocity, causing them to then interact with the magnetic field vector of said radiation beam via a v×B ponderomotive force, thereby deflecting said charged particles in the direction of said propagating radiation beam and causing the transverse velocity vectors of said charged particles to remain in near synchronism with the electric field vector of said traveling wave and thereby continue to gain energy until said charged particles leave said high field focal region.
Claim 3
Dependent Claim
46 words
An apparatus according to claim 1 wherein a Rayleigh region and focal spot region are chosen to provide maximum acceleration by iteratively adjusting said focal region to match the region of acceleration, with said region determined by the electric field strengths attainable at the focal plane.
Claim 4
Dependent Claim
28 words
A device according to claim 1 wherein the said particle stream is comprised of electrons injected coaxial to a laser beam with velocities approaching the speed of light.
Claim 5
Dependent Claim
30 words
A device according to claim 1 wherein the said particle stream or streams is comprised of electrons injected normal to a laser beam with velocities adjusted to produce maximum acceleration.
Claim 6
Dependent Claim
17 words
A device according to claim 1 wherein the intense traveling electromagnetic waves are linearly or circularly polarized.
Claim 7
Dependent Claim
34 words
An apparatus according to claim 1 wherein said focal region of the traveling electromagnetic waves is internal to the source, such as inside a laser resonator cavity, where power levels are at a maximum.
Claim 8
Dependent Claim
47 words
An apparatus to claim 1 wherein the intense traveling electromagnetic waves are periodically refocussed to produce multiple acceleration regions which can act upon previously accelerated particles which are also refocussed, or accelerate newly injected particles to produce multiple beams which may be combined downstream of the accelerator.
Claim 9
Dependent Claim
34 words
An apparatus according to claim 1 wherein the source of the intense traveling electromagnetic waves operates in the microwave region, and the required focusing is accomplished via a quasi-optical cavity or dielectric lens array.
Claim 10
Dependent Claim
59 words
An apparatus according to claim 1 wherein a solenoidal magnetic field coaxial to the electromagnetic wave is provided to constrain or focus the accelerated charged particles prior to extraction, with said solenoidal magnetic field also serving to extend the length of time the particles remain in near synchronism with the traveling waves, thus allowing higher energies to be attained.
References Cited (Backward Citations)
US3267383A
Cited
US3450931A
Cited
US3622833A
Cited
US3463959A
Cited
US3730979A
Cited
US3860880A
Cited
US4215291A
Cited
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1989-02-10 | 1989-08-12 | 1990-02-11 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1993-02-10 | 1993-08-12 | 1994-02-11 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1997-02-10 | 1997-08-12 | 1998-02-11 | $7700.00 | Window Closed / Lapsed |