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US 6,285,690 B1Granted
Ignition feedback regenerative free electron laser (FEL) amplifier
AssigneeBennett Optical Research, Inc.
InventorsKwang-Je Kim, Alexander Zholents, Max Zolotorev
Life of this patent
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Abstract
An ignition feedback regenerative amplifier consists of an injector, a linear accelerator with energy recovery, and a high-gain free electron laser amplifier. A fraction of the free electron laser output is coupled to the input to operate the free electron laser in the regenerative mode. A mode filter in this loop prevents run away instability. Another fraction of the output, after suitable frequency up conversion, is used to drive the photocathode. An external laser is provided to start up both the amplifier and the injector, thus igniting the system.
Claims64
An ignition feedback regenerative FEL amplifier comprising:
- A. An ignition laser which emits optical pulses along a predetermined path;
- B. an up converter placed in said optical pulse path, said up converter designed to change the wavelength of said optical pulses to a predetermined wavelength pulse;
- C. an injector placed in the path of said changed wavelength pulse such that an a electron bunch of a preselected energy is emitted in response to each of said pulses of predetermined wavelength, quality, and power level;
- D. a linear accelerator in the path of said electron bunch, said linear accelerator increases the energy contained in said electron bunches such that upon exiting said linear accelerator enhanced electron bunches are emitted;
- E. a bunch compressor around the path of said enhanced electron bunches such that said enhanced electron bunches are directed into a predetermined direction as a compressed electron bunch;
- F. an undulator placed in the path of said compressed electron bunches traveling along said predetermined direction, said undulator functioning as a free electron laser amplifier for said compressed electron bunches such that an optical beam is emitted from said undulator for each of said compressed electron bunches;
- G. a first dividing means in the path of said optical beam emitted from said undulator for directing a predetermined portion of said optical beam back into said injector via said up converter to change the wavelength of said portion of said optical beam from said undulator to initial a new electron pulse, said new electron pulse having an intensity determined by the power level of said portion of said optical beam from said first dividing means, said predetermined portion of said optical beam is set at a level which generates a larger electron bunch from said injection which in turn gives a higher energy optical beam from said undulator, and in turn said predetermined portion of said optical beam increases due to said higher energy optical beam, thus an increasing feedback situation has been created;
- H. a second dividing means in the path of said optical beam emitted from said undulator for looping a portion of said optical beam back to said undulator so as to enter at the same time as a compressed electron bunch enters said undulator;
- I. a plurality of mirrors placed to direct said optical beam portion created by said second dividing means back into said undulator so as to enhance optical emission of a compressed electron bunch while in said undulator;
- J. a mode filter placed in the path of said beam portion created by said second dividing means for stopping passage of said optical beam beyond a preset power level;
- K. a bunch decompressor around the path of said compressed electron bunches after they have passed through said undulator such that said electron bunches are redirected into said linear accelerator a second time after being decompressed so as to be decelerated by said linear accelerator;
- and
- L. a beam dump aligned to receive said decompressed electron bunch after it has been decelerated by passage through said linear accelerator said second time.
10 more elements
An ignition feedback regenerative FEL amplifier comprising:
- A. An ignition laser which emits a first and a second optical pulses along a predetermined path;
- B. an up converter placed in said first optical pulse path, said up converter designed to change the wavelength of said first optical pulses to a predetermined wavelength pulse;
- C. an injector placed in the path of said changed wavelength pulse such that an electron bunch of a preselected energy is emitted in response to each of said pulses of predetermined wavelength, quality, and power level;
- D. a linear accelerator in the path of said electron bunch, said linear accelerator increases the energy contained in said electron bunches such that upon exiting said linear accelerator enhanced electron bunches are emitted;
- E. a bunch compressor around the path of said enhanced electron bunches such that said enhanced electron bunches are directed into a predetermined direction as a compressed electron bunch;
- F. an undulator placed in the path of said compressed electron bunches traveling along said predetermined direction, said undulator functioning as a free electron laser amplifier for said compressed electron bunches such that an optical beam is emitted from said undulator for each of said compressed electron bunches;
- G. a first dividing means in the path of said optical beam emitted from said undulator for directing a predetermined portion of said optical beam back into said injector via said up converter to change the wavelength of said portion of said optical beam from said undulator to initial a now electron pulse, said new electron pulse having an intensity determined by the power level of said portion of said optical beam from said first dividing means, said predetermined portion of said optical beam is set at a level which generates a larger electron bunch from said injector which in turn gives a higher energy optical beam from said undulator, and in turn said predetermined portion of said optical beam increases due to said higher energy optical beam, thus an increasing feedback situation has been created;
- H. a second dividing means in the path of said optical beam emitted from said undulator for looping a portion of said optical beam back to said undulator so as to enter at the same time as a compressed electron bunch enters said undulator;
- I. a plurality of mirrors placed to direct said optical beam portion created by said second dividing means back into said undulator so as to enhance optical emission of a compressed electron bunch while in said undulator;
- J. a mode filter placed in the path of said beam portion created by said second dividing means for stopping passage of said optical beam beyond a preset power level;
- K. a bunch decompressor around the path of said compressed electron bunches after they have passed through said undulator such that said electron bunches are redirected into said linear accelerator a second time after being decompressed so as to be decelerated by said linear accelerator;
- L. an optical path for said second optical pulse from said ignition laser which directs said second optical pulse into said undulator at the same time as said compressed electron bunch enters said undulator;
- and
- M. a beam dump aligned to receive said decompressed electron bunch after it has been decelerated by passage through said linear accelerator said second time.
11 more elements
Dependencies are inferred from the claim text.