RF Control System for the NLC Linacs

RF Control System for the NLC Linacs PDF Author:
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Languages : en
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The proposed Next Linear Collider contains a large number of linac RF systems with new requirements for wideband klystron modulation and accurate RF vector detection. The system will be capable of automatically phasing each klystron and compensating for beam loading effects. Accelerator structure alignment is determined by detection of the beam induced dipole modes with a receiver similar to that used for measuring the accelerator RF and is incorporated into the RF system topology. This paper describes the proposed system design, signal processing techniques and includes preliminary test results.

RF Control System for the NLC Linacs

RF Control System for the NLC Linacs PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
The proposed Next Linear Collider contains a large number of linac RF systems with new requirements for wideband klystron modulation and accurate RF vector detection. The system will be capable of automatically phasing each klystron and compensating for beam loading effects. Accelerator structure alignment is determined by detection of the beam induced dipole modes with a receiver similar to that used for measuring the accelerator RF and is incorporated into the RF system topology. This paper describes the proposed system design, signal processing techniques and includes preliminary test results.

חקר רמות מעוררות בגרעין I131

חקר רמות מעוררות בגרעין I131 PDF Author:
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Languages : en
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STATUS OF A LINAC RF UNIT DEMONSTRATIONFOR THE NLC

STATUS OF A LINAC RF UNIT DEMONSTRATIONFOR THE NLC PDF Author:
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Languages : en
Pages : 5

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Designs for a future TeV scale electron-positron X-band linear collider (NLC/GLC) require main linac units which produce and deliver 450 MW of rf power at 11.424 GHz to eight 60 cm accelerator structures. The design of this rf unit includes a SLED-II pulse compression system with a gain of approximately three at a compression ratio of four, followed by an over-moded transmission and distribution system. We have designed, constructed, and operated such a system as part of the 8-Pack project at SLAC. Four 50 MW X-band klystrons, running off a common 400 kV solid-state modulator, drive a dual-moded SLED-II pulse compression system. The compressed power is delivered to structures in the NLCTA beamline. Four 60 cm accelerator structures are currently installed and powered, with four additional structures and associated high power components available for installation late in 2004. We describe the layout of our system and the various high-power components which comprise it. We also present preliminary data on the processing and initial high-power operation of this system.

The RF Phase Distribution and Timing System for the NLC.

The RF Phase Distribution and Timing System for the NLC. PDF Author:
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Languages : en
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The Next Linear Collider accelerator will require phase synchronization of (approximately) 20°X-band (11.424 GHz) long term, and (approximately) 1°X-band short term throughout its 30 kilometer length. A prototype fiber optic distribution system has been constructed to demonstrate this level of performance. This system operates by measuring the optical round trip time in the fiber, and then controlling the fiber phase length to stabilize this measurement. The authors describe the design of this system, and show recent results on stability and phase noise.

Digital RF Control System for the Pulsed Superconducting Linear Accelerator

Digital RF Control System for the Pulsed Superconducting Linear Accelerator PDF Author: Valeri Ayvazyan
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Category : Technology
Languages : en
Pages :

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Book Description
Digital RF Control System for the Pulsed Superconducting Linear Accelerator.

Beam-based Feedback Simulations for the NLC Linac

Beam-based Feedback Simulations for the NLC Linac PDF Author:
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Languages : en
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Book Description
Extensive beam-based feedback systems are planned as an integral part of the Next Linear Collider (NLC) control system. Wakefield effects are a significant influence on the feedback design, imposing both architectural and algorithmic constraints. Studies are in progress to assure the optimal selection of devices and to refine and confirm the algorithms for the system design. The authors show the results of initial simulations, along with evaluations of system response for various conditions of ground motion and other operational disturbances.

Design and Evaluation of a Low-level RF Control System Analog

Design and Evaluation of a Low-level RF Control System Analog PDF Author:
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Languages : en
Pages : 29

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Book Description
The proposed RF distribution scheme for the two 15 km long ILC LINACs, uses one klystron to feed 26 superconducting RF cavities operating at 1.3 GHz. For a precise control of the vector sum of the signals coming from the SC cavities, the control system needs a high performance, low cost, reliable and modular multichannel receiver. At Fermilab we developed a 96 channel, 1.3 GHz analog/digital receiver for the ILC LINAC LLRF control system. In the paper we present a balanced design approach to the specifications of each receiver section, the design choices made to fulfill the goals and a description of the prototyped system. The design is tested by measuring standard performance parameters, such as noise figure, linearity and temperature sensitivity. Measurements show that the design meets the specifications and it is comparable to other similar systems developed at other laboratories, in terms of performance.

A New Approach in Simulating RF Linacs Using a General, Real-time Signal Processor

A New Approach in Simulating RF Linacs Using a General, Real-time Signal Processor PDF Author:
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Category :
Languages : en
Pages : 4

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Book Description
Strict requirements on the tolerances of the amplitude and phase of the radio frequency (RF) cavity field have recently been necessary to advance the field of accelerator technology. Due to these stringent requirements of modern accelerators a new approach of modeling and simulating is essential in developing and understanding their characteristics. This paper describes the implementation of a general, linear model of an RF cavity which is used to develop a real-time signal processor. This device fully emulates the response of an RF cavity upon receiving characteristic parameters (Q0, [omega]0, [delta][omega], R{sub S}, [zeta]0). Simulating an RF cavity with real-time signal processor is beneficial to accelerator designers because the device allows one to answer fundamental questions on the response of the cavity to a particular stimulus without running the accelerator. In particular, the complex interactions between the RF power and the control systems, the beam and cavity fields can simply be observed in a real-time domain. The signal processor can also be used upon initialization of the accelerator as a diagnostic device and as a dummy load for determining the closed loop error of the system. In essence, the signal processor is capable of determining whether the control systems and peripheral devices are operating properly without going through the tedious procedure of running beam through a cavity.

DESIGN OF THE RF PHASE AND AMPLITUDE CONTROL SYSTEM FOR A PROTON LINEAR ACCELERATOR.

DESIGN OF THE RF PHASE AND AMPLITUDE CONTROL SYSTEM FOR A PROTON LINEAR ACCELERATOR. PDF Author:
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Languages : en
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SYSTEM IDENTIFICATION OF THE LINAC RF SYSTEM USING A WAVELET METHOD AND ITS APPLICATIONS IN THE SNS LLRF CONTROL SYSTEM.

SYSTEM IDENTIFICATION OF THE LINAC RF SYSTEM USING A WAVELET METHOD AND ITS APPLICATIONS IN THE SNS LLRF CONTROL SYSTEM. PDF Author:
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Languages : en
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For a pulsed LINAC such as the SNS, an adaptive feed-forward algorithm plays an important role in reducing the repetitive disturbance caused by the pulsed operation conditions. In most modern feed-forward control algorithms, accurate real time system identification is required to make the algorithm more effective. In this paper, an efficient wavelet method is applied to the system identification in which the Haar function is used as the base wavelet. The advantage of this method is that the Fourier transform of the Haar function in the time domain is a sine function in the frequency domain. Thus we can directly obtain the system transfer function in the frequency domain from the coefficients of the time domain system response.