Experimental Beam Dynamics in the SLC (SLAC Linear Collier) Linac

Experimental Beam Dynamics in the SLC (SLAC Linear Collier) Linac PDF Author:
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ISBN:
Category :
Languages : en
Pages :

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Book Description
The component installation for the upgrade of the three-kilometer linac for the SLAC Linear Collider (SLC) was completed in late summer 1986. The system status and measurements of beam properties made during commissioning are described in this paper. In summary, a low-emittance electron beam from a damping ring has been accelerated through the linac and injected into the north SLC Arc with negligible loss. The maximum bunch intensity is 2.9 x 10 electrons/pulse. A peak particle energy of 53 GeV has been reached. Operation at 47 GeV is now routine. The energy and energy spectrum of the electron beam can be rapidly measured nondestructively at high energy. These signals will be used in a fast feedback system nearing completion. The electron beam can be centered in the accelerator to about 200 m rms. Slow feedback of the injection position and angle into the linac and injection into the north Arc are operational. Longitudinal and transverse wakefields have been measured and appear to be near expectations. Transverse position measurements at the end of the linac show a 120 m horizontal and a 30 m vertical (rms) jitter from pulse to pulse. The spot shape, including the transverse tails, also shows some jitter. The transverse position and shape fluctuations have several sources involving launch instabilities, chromatic effects, RF deflections and lattice mismatches. Continued improvements are expected. These parameter jitters would not preclude collisions. The measured invariant transverse emittances of the beam at 47 GeV are 2 x 10 V rm vertically and 12-25 x 10 V rm horizontally at 1 x 10 e . The horizontal emittance increases with beam intensity. Damped positrons have been injected into the linac, and trajectory correction is underway.

Experimental Beam Dynamics in the SLC (SLAC Linear Collier) Linac

Experimental Beam Dynamics in the SLC (SLAC Linear Collier) Linac PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
The component installation for the upgrade of the three-kilometer linac for the SLAC Linear Collider (SLC) was completed in late summer 1986. The system status and measurements of beam properties made during commissioning are described in this paper. In summary, a low-emittance electron beam from a damping ring has been accelerated through the linac and injected into the north SLC Arc with negligible loss. The maximum bunch intensity is 2.9 x 10 electrons/pulse. A peak particle energy of 53 GeV has been reached. Operation at 47 GeV is now routine. The energy and energy spectrum of the electron beam can be rapidly measured nondestructively at high energy. These signals will be used in a fast feedback system nearing completion. The electron beam can be centered in the accelerator to about 200 m rms. Slow feedback of the injection position and angle into the linac and injection into the north Arc are operational. Longitudinal and transverse wakefields have been measured and appear to be near expectations. Transverse position measurements at the end of the linac show a 120 m horizontal and a 30 m vertical (rms) jitter from pulse to pulse. The spot shape, including the transverse tails, also shows some jitter. The transverse position and shape fluctuations have several sources involving launch instabilities, chromatic effects, RF deflections and lattice mismatches. Continued improvements are expected. These parameter jitters would not preclude collisions. The measured invariant transverse emittances of the beam at 47 GeV are 2 x 10 V rm vertically and 12-25 x 10 V rm horizontally at 1 x 10 e . The horizontal emittance increases with beam intensity. Damped positrons have been injected into the linac, and trajectory correction is underway.

Beam Dynamics Verification in Linacs of Linear Colliders

Beam Dynamics Verification in Linacs of Linear Colliders PDF Author:
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ISBN:
Category :
Languages : en
Pages :

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Book Description
The SLAC two-mile linac has been upgraded to accelerate high current, low emittance electron and positron beams to be used in the SLAC Linear Collider (SLC). After the upgrade was completed, extensive beam studies were made to verify that the design criteria have been met. These tests involved the measurement of emittance, beam phase space orientation, energy dispersion, trajectory oscillations, bunch length, energy spectrum and wakefields. The methods, the systems and the data cross checks are compared for the various measurements. Implications for the next linear collider are discussed. 12 refs., 13 figs., 2 tabs.

Energy Research Abstracts

Energy Research Abstracts PDF Author:
Publisher:
ISBN:
Category : Power resources
Languages : en
Pages : 716

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Proceedings of the SLC Workshop on Experimental Use of the SLAC Linear Collider

Proceedings of the SLC Workshop on Experimental Use of the SLAC Linear Collider PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 257

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Proceedings of the SLC Workshop on Experimental Use of the SLAC Linear Collider

Proceedings of the SLC Workshop on Experimental Use of the SLAC Linear Collider PDF Author:
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ISBN:
Category : Colisiones (FĂ­sica nuclear)
Languages : en
Pages : 646

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Linear Accelerator Beam Dynamics

Linear Accelerator Beam Dynamics PDF Author: Wolfgang Kurt Hermann Panofsky
Publisher:
ISBN:
Category : Beam dynamics
Languages : en
Pages : 24

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Short High Charge Bunches in the SLAC Linac

Short High Charge Bunches in the SLAC Linac PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 5

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Book Description
The linac at the Stanford Linear Accelerator Center (SLAC) can provide beams to different experiments during PEP-II operations. It is planned to have a 30-GeV beam to the end of the linac into the FFTB (Final Focus Test Beam) area, where there will be two plasma experiments installed. They will demonstrate plasma focusing and plasma acceleration up to 1 GeV/m. The acceleration goes linear with the current and is inversely proportional to the square of the bunch length. These high charge, short bunches will create strong longitudinal wakefields in the linac. They create a strong double-horned energy profile and have different beam dynamics in the linac. Therefore we made a test run in Fall of 1998 to measure and quantify the beam properties, like stability, distributions, tails, and backgrounds, which will be discussed in this paper. The actual plasma experiments are planned for the spring of 1999.

Acceleration of High Charge Density Electron Beams in the SLAC Linac

Acceleration of High Charge Density Electron Beams in the SLAC Linac PDF Author:
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ISBN:
Category :
Languages : en
Pages :

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Book Description
The SLAC Linear Collider (SLC) will require both electron and positron beams of very high charge density and low emittance to be accelerated to about 50 GeV in the SLAC 3-km linac. The linac is in the process of being improved to meet this requirement. The program to accelerate an electron beam of high charge density through the first third of the SLC linac is described and the experimental results are discussed. 7 references, 5 figures.

SLAC Linear Collider

SLAC Linear Collider PDF Author: Stanford Linear Accelerator Center
Publisher:
ISBN:
Category : Linear accelerators
Languages : en
Pages : 208

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Beam Dynamics in SLC.

Beam Dynamics in SLC. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 7

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Book Description
Beam dynamics issues affect many different aspects of the SLC performance. This paper concentrates on the multi-particle beam dynamics in the linac and the associated limitations that are imposed on the overall SLC performance. The beam behavior in the presence of strong wakefields has been studied in order to optimize the performance and to predict the expected emittances in high performance linacs. Emittance measurements and simulations are presented for the SLAC linac and are compared in detail. As the overall SLC performance depends on the accelerator stability, the tuning stability is discussed. Measurements are shown and the consequences for the performance of the SLC are discussed.