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By D. A. Edwards

The 1st part offers with the movement of a unmarried particle less than the impact of digital and magnetic fields. the elemental language of linear and round accelerators is built. the primary of section balance is brought besides part oscillations in linear accelerators and synchrotrons. provides a therapy of betatron oscillations through an day trip into nonlinear dynamics and its program to accelerators. the second one part discusses depth established results, really house cost and coherent instabilities. contains tables of parameters for a variety of accelerators that are utilized in the varied difficulties supplied on the finish of every bankruptcy.

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D. Drechsel, O. S. Kamalov, and L. Tiator, Nucl. Phys. A 645, 145 (1999). de/MAID/. 18. M. Warns, H. Schroder, W. Pfeil, and H. Rollnik, Z. Phys. C 45, 627 (1990). 19. G. Aznauryan, Z. Phys. A 346, 297 (1993). 20. Th. Pospischil et al, Phys. Rev. Lett. 86, 2959 (2001). 21. C. Mertz et al, Phys. Rev. Lett. 86, 2963 (2001). 22. F. Kalleicher et al, Z. Phys. A 359, 201 (1997). RECOIL POLARIZATION M E A S U R E M E N T S IN TV° E L E C T R O P R O D U C T I O N AT T H E P E A K OF T H E A(1232) A. J.

The model calculations are those of SatoLee 1 4 and MAID. We were able to access the low momentum branch of the recoiling protons by tuning the OOPS spectrometers to very low momentum detection. We were able to thus access 8*q = 151° and at 8*q = 180° for an RLT measurement. The high duty-cycle extracted beam also provided a significant advantage for studies of the TT+ channel dramatically reducing the experimental background. 5°. All three unpolarized response functions could be determined. In addition we measured the cross section in parallel kinematics.

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