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Abstract:
The principle for measuring the loss impedance of a storage ring,which is caused by the energy loss of the stored bunched beam in passing through discontinuous parts of the vacuum chamber of the ring,is discussed and the set up to measure the loss impedance of HESYRL storage ring is described.
The measurement results of the energy loss and loss impedance of the dicker vacuum chamber,the septum vacuum chamber and other parts to be installed on the HESYRL storage ring are given.Some of the results are consistent with those measured in DESY.
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References
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M. Sands, "Energy Loss to Parasitic Modes of the Accelerating cavities", PEP-90 (July 25, 1974).[2] M. Sands and J. Rees, "A Bench Measurement of the Energy Loss of a Stored Beam to a Cavity", PEP-95(August 1974).[3] J. Peters, "Bench Measurements of the Energy Loss of a Stored Beam to Vacuum Components", IEEE Trans.,Vol. NS-24, No. 3, (June 1977).[4] P. B. Wilson, J. B. Styles and K. L. F. Bane, "Comparison of Measured and Computed Loss to ParasiticModes in Cylindrical Cavities with Beam Ports", PEP-240 (March 1977).[5] M. G. Billing, J . L. Kirchgessner and R. M. Sundelin, "Simulation Measurement of Bunch Excited Fieldsand Energy Loss in Vacuum Chamber Components and Cavities", IEEE Trans., Vol. NS-26, No. 3 (June1979).[6] J. W. Wang, G. A. Loew, J. N. Weaver and P. B. Wilson, "Microwave Measurements of Energy Loss toLongitudinal Modes by Single Electron Bunches Traversing Periodic Structures", SLAC-PUB-2830 (October1981).[7] J. N. Weaver, "Measuring, Calculating and Estimating PEP'S Parasitic Mode Loss Parameters", PEP-NOTE-342 (January 1981). |
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