Measurements of the beam emittance during bunch compression in the CLIC Test Facility (CTF-II) are described. The measurements were made with different beam charges and different energy correlations versus the bunch compressor settings which were varied from no compression through the point of full compression and to over-compression. Significant increases in the beam emittance were observed with the maximum emittance occuring near the point of full (maximal) compression. Finally, evaluation of possible emittance dilution mechanisms indicate that coherent synchrotron radiation was the most likely cause
The bunch compressor of the A0 Photoinjector at Fermilab was removed this past spring to install a t...
In order to reach the high peak current required for an x-ray free electron laser, two separate magn...
The Linac Coherent Light Source (LCLS) is a SASE xray free-electron laser project presently under co...
Bunches of high charge (10 nC) are compressed in length in the CTF II bunch compressor from 1.2 mm r...
Bunches of high charge (10 nC) are compressed in length in the CTF II bunch compressor from 1.2 mm r...
Bunches of high charge (10 nC) are compressed in length in the CTF II bunch compressor from 1.2 mm r...
Bunches of high charge (up to 10 nC) are compressed in length in the CTF II magnetic chicane to less...
Minimizing the dilution of the electron beam emittance is crucial for the performance of accelerator...
Minimizing the dilution of the electron beam emittance is crucial for the performance of accelerator...
Minimizing the dilution of the electron beam emittance is crucial for the performance of accelerator...
Electron bunches of high charge (up to 10 nC) are compressed in length in the Compact Linear Collide...
Evolution of short intense electron bunches passing through bunch-compressing beam lines is studied ...
The Test Facility of the "Compact Linear Collider" (CLIC) at CERN (CTF), has to prove the feasibilit...
Evolution of short intense electron bunches passing through bunch-compressing beam lines is studied ...
The drive beam of CTF II can provide single electron bunches with charges of more than 15 nC and rms...
The bunch compressor of the A0 Photoinjector at Fermilab was removed this past spring to install a t...
In order to reach the high peak current required for an x-ray free electron laser, two separate magn...
The Linac Coherent Light Source (LCLS) is a SASE xray free-electron laser project presently under co...
Bunches of high charge (10 nC) are compressed in length in the CTF II bunch compressor from 1.2 mm r...
Bunches of high charge (10 nC) are compressed in length in the CTF II bunch compressor from 1.2 mm r...
Bunches of high charge (10 nC) are compressed in length in the CTF II bunch compressor from 1.2 mm r...
Bunches of high charge (up to 10 nC) are compressed in length in the CTF II magnetic chicane to less...
Minimizing the dilution of the electron beam emittance is crucial for the performance of accelerator...
Minimizing the dilution of the electron beam emittance is crucial for the performance of accelerator...
Minimizing the dilution of the electron beam emittance is crucial for the performance of accelerator...
Electron bunches of high charge (up to 10 nC) are compressed in length in the Compact Linear Collide...
Evolution of short intense electron bunches passing through bunch-compressing beam lines is studied ...
The Test Facility of the "Compact Linear Collider" (CLIC) at CERN (CTF), has to prove the feasibilit...
Evolution of short intense electron bunches passing through bunch-compressing beam lines is studied ...
The drive beam of CTF II can provide single electron bunches with charges of more than 15 nC and rms...
The bunch compressor of the A0 Photoinjector at Fermilab was removed this past spring to install a t...
In order to reach the high peak current required for an x-ray free electron laser, two separate magn...
The Linac Coherent Light Source (LCLS) is a SASE xray free-electron laser project presently under co...