Beam Parametr Measurements for the SLAC Linear Collider

Beam Parametr Measurements for the SLAC Linear Collider PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
A stable, closely-controlled, high-intensity, single-bunch beam will be required for the SLAC Linear Collider. The characteristics of short-pulse, low-intensity beams in the SLAC linac have been studied. A new, high-intensity thermionic gun, subharmonic buncher and S-band buncher/accelerator section were installed recently at SLAC. With these components, up to 1011 electrons in a single S-band bunch are available for injection into the linac. the first 100-m accelerator sector has been modified to allow control of short-pulse beams by a model-driven computer program. Additional instrumentation, including a computerized energy analyzer and emittance monitor have been added at the end of the 100-m sector. The beam intensity, energy spectrum, emittance, charge distribution and the effect of wake fields in the first accelerator sector have been measured. The new source and beam control system are described and the most recent results of the beam parameter measurements are discussed.

Beam Parametr Measurements for the SLAC Linear Collider

Beam Parametr Measurements for the SLAC Linear Collider PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
A stable, closely-controlled, high-intensity, single-bunch beam will be required for the SLAC Linear Collider. The characteristics of short-pulse, low-intensity beams in the SLAC linac have been studied. A new, high-intensity thermionic gun, subharmonic buncher and S-band buncher/accelerator section were installed recently at SLAC. With these components, up to 1011 electrons in a single S-band bunch are available for injection into the linac. the first 100-m accelerator sector has been modified to allow control of short-pulse beams by a model-driven computer program. Additional instrumentation, including a computerized energy analyzer and emittance monitor have been added at the end of the 100-m sector. The beam intensity, energy spectrum, emittance, charge distribution and the effect of wake fields in the first accelerator sector have been measured. The new source and beam control system are described and the most recent results of the beam parameter measurements are discussed.

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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Single Bunch Beam Measurements for the Proposed SLAC Linear Collider

Single Bunch Beam Measurements for the Proposed SLAC Linear Collider PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
Single S-band bunches of approx. 109 electrons have been used to study the characteristics of the SLAC linac in anticipation of its operation as a linear collider. Emittance measurements have been made, the longitudinal charge distribution within single bunches has been determined and transverse emittance growth has been produced by deliberately missteering the beam. New equipment is being installed and checked out, and the sensitivity of new traveling-wave beam position monitors has been measured.

Beam Size Measurement at High Radiation Levels

Beam Size Measurement at High Radiation Levels PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 3

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Book Description
At the end of the Stanford Linear Accelerator the high energy electron and positron beams are quite small. Beam sizes below 100 [mu]m ([sigma]) as well as the transverse distribution, especially tails, have to be determined. Fluorescent screens observed by TV cameras provide a quick two-dimensional picture, which can be analyzed by digitization. For running the SLAC Linear Collider (SLC) with low backgrounds at the interaction point, collimators are installed at the end of the linac. This causes a high radiation level so that the nearby cameras die within two weeks and so-called radiation hard'' cameras within two months. Therefore an optical system has been built, which guides a 5 mm wide picture with a resolution of about 30 [mu]m over a distance of 12 m to an accessible region. The overall resolution is limited by the screen thickness, optical diffraction and the line resolution of the camera. Vibration, chromatic effects or air fluctuations play a much less important role. The pictures are colored to get fast information about the beam current, size and tails. Beside the emittance, more information about the tail size and betatron phase is obtained by using four screens. This will help to develop tail compensation schemes to decrease the emittance growth in the linac at high currents. 4 refs., 2 figs.

Energy Research Abstracts

Energy Research Abstracts PDF Author:
Publisher:
ISBN:
Category : Power resources
Languages : en
Pages : 444

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Measurement and Control of Charged Particle Beams

Measurement and Control of Charged Particle Beams PDF Author: Michiko G. Minty
Publisher: Springer Science & Business Media
ISBN: 366208581X
Category : Science
Languages : en
Pages : 364

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Book Description
From the reviews: "This book is a very welcome and valuable addition to the accelerator literature. As noted by the authors, there is relatively little material in the book specifically for low-energy machines, but industrial users may still find it useful to read." Cern Courier

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 : Colisiones (FĂ­sica nuclear)
Languages : en
Pages : 646

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Beam Line

Beam Line PDF Author:
Publisher:
ISBN:
Category : Particle beams
Languages : en
Pages : 460

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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:
Publisher:
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.