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Wakefield dependent emittance growth in the SLAC (Stanford Linear Accelerator Center) linac

K. Bane

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Abstract

In this note we describe the emittance growth we can expect at bunch populations of N = 3,4,5 {times} 10{sup 10} in the SLC linac. We will discuss briefly the effects of injection jitter, injection drift, and coherent oscillations starting in the middle of the linac. Finally, we will discuss in a more thorough manner the effects of random misalignment errors throughout the linac.

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In this note we describe the emittance growth we can expect at bunch populations of N = 3,4,5 {times} 10{sup 10} in the SLC linac. We will discuss briefly the effects of injection jitter, injection drift, and coherent oscillations starting in the middle of the linac. Finally, we will discuss in a more thorough manner the effects of random misalignment errors throughout the linac.

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Available abstract

In this note we describe the emittance growth we can expect at bunch populations of N = 3,4,5 {times} 10{sup 10} in the SLC linac. We will discuss briefly the effects of injection jitter, injection drift, and coherent oscillations starting in the middle of the linac. Finally, we will discuss in a more thorough manner the effects of random misalignment errors throughout the linac.

Key concepts: Linear particle accelerator, Thermal emittance, Physics, Particle accelerator, Jitter, Nuclear physics, Optics, Beam (structure)

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