Laser acceleration system for generating monoenergetic protons
First Claim
1. A proton acceleration system for accelerating protons within a target comprising:
- a laser source generating a laser beam having a wavelength λ
L and intensity; and
a target formed of foil having a selected thickness, wherein the target irradiated by the laser beam and transformed into a plasma having a target density causing a treatment energy to be emitted from the foil due to the irradiation;
wherein the thickness of the foil of the target is selected so that the foil has a thickness within a range of optimal thickness Δ
s to 2×
Δ
s, wherein Δ
s is less than the laser wavelength and is a function of the laser intensity, laser wavelength, and target density sufficient to achieve radiation pressure acceleration (RPA).
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Abstract
A proton acceleration system is provided for accelerating protons within a target. The system includes a laser source generating a laser beam having a wavelength λL and intensity and a target formed of foil having a selected thickness. The target is irradiated by the laser beam and transformed into a plasma that has a target density. This causes a treatment energy to be emitted from the foil due to the irradiation. The thickness of the foil of the target is selected so that the foil has a thickness within a range of optimal thickness Δs to 2×Δs, wherein Δs is less than the laser wavelength and is a function of the laser intensity, laser wavelength, and target density sufficient to achieve radiation pressure acceleration (RPA).
34 Citations
34 Claims
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1. A proton acceleration system for accelerating protons within a target comprising:
-
a laser source generating a laser beam having a wavelength λ
L and intensity; anda target formed of foil having a selected thickness, wherein the target irradiated by the laser beam and transformed into a plasma having a target density causing a treatment energy to be emitted from the foil due to the irradiation; wherein the thickness of the foil of the target is selected so that the foil has a thickness within a range of optimal thickness Δ
s to 2×
Δ
s, wherein Δ
s is less than the laser wavelength and is a function of the laser intensity, laser wavelength, and target density sufficient to achieve radiation pressure acceleration (RPA). - View Dependent Claims (2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22, 23, 24, 25)
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26. A controller for a proton acceleration system including a laser source generating a pulsed laser beam having a wavelength λ
-
L and intensity; and
further including a target formed of foil which is irradiated by the laser beam and transformed into a plasma having a target density causing a treatment energy to be emitted from the foil due to the irradiation, wherein the controller comprising;a tangible processor; and a memory with instructions to be executed by the tangible processor for selecting a thickness of the foil of the target so that the foil has a thickness within a range of optimal thickness Δ
s to 2×
Δ
s, wherein Δ
s is less than the laser wavelength and is a function of the laser intensity, laser wavelength, and target density sufficient to achieve radiation pressure acceleration (RPA). - View Dependent Claims (27, 28, 29, 30, 31, 32)
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L and intensity; and
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33. A method for controlling a proton acceleration system including a laser source generating a pulsed laser beam having a wavelength λ
-
L and intensity; and
further including a target formed of foil which is irradiated by the laser beam and transformed into a plasma having a target density causing a treatment energy to be emitted from the foil due to the irradiation comprising;selecting a thickness of the foil of the target so that the foil has a thickness within a range of optimal thickness Δ
s to 2×
Δ
s, wherein Δ
s is less than the laser wavelength and is a function of the laser intensity, laser wavelength, and target density sufficient to achieve radiation pressure acceleration (RPA). - View Dependent Claims (34)
-
L and intensity; and
Specification