STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA

STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA

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FIG. 5.1: Successive frames in time (progressing from left to right) from a movie of the synchrotron light monitor in the second endloop at the onset of BBU. 5.1 Overview While the remainder of this chapter is dedicated to describing the details of the quantitative measurements, Fig. 5.1 illustrates a qualitative characterization of BBU. Figure 5.1 shows a series of frames from a recording of a synchrotron light monitor located in the second recirculation arc of the FEL Driver. During the recording, the average beam current was being slowly increased until beam breakup developed. The instability clearly manifests itself as vertical growth which continues until beam losses become large enough to trip the machine off. The time elapsed from the first to the last frame of Fig. 5.1 is approximately 0.25 s. From the point of view of a machine operator in the control room, the only indication that the operating current is approaching the threshold current are obser- vations of the SLM image growing as depicted in Fig. 5.1. Additional characteristics of the presence of BBU - from an operator’s perspective - are single, hard machine trips at one particular beam loss monitor (BLM) location. In most instances, these BLM trips occurred in the 5F region of the Driver where the recirculated beam is re-injected through the linac and the beam envelopes are largest. Clearly a more quantitative method is needed to confirm that a machine trip is due to BBU. Additional measurements are required to ascertain which cavity contains the dangerous HOM and to determine the frequency of the mode. Fur- 113 thermore, adequately benchmarking BBU codes requires accurately measuring the

threshold current - preferably with several different methods for consistency. All these measurements require the ability to measure one of the signatures of BBU, namely the HOM power. 5.2 HOM Power Measuring the HOM power proved to be ideal in regards to studying BBU and was achieved using Schottky diodes [77]. Several attempts to measure the response of BPM striplines, to see the exponentially growing displacement due to the instability, were unsuccessful. Ultimately, the HOM power is easier to monitor and provides a signal that is robust enough to make a number of independent measurements as discussed in Sections 5.4.3 and 5.4.4. The key element in all these measurements is the fact that the cavities in the zone 3 cryomodule, unlike previous CEBAF 5-cell cavities, use DESY-like coaxial HOM couplers [75]. Cables connected to the HOM ports are loaded on 50 Ω resistors. In order to monitor the HOM power a small portion of the signal from each HOM port is directed to a Schottky diode by a −20 dB directional coupler. The output of each diode is connected to a separate oscilloscope channel. This allows the HOM power to be individually monitored from each of the 8 cavities. The Schottky diode assembly is shown in Fig. 5.2. 5.2.1 Schottky Diodes A Schottky diode acts as a rectifier, converting an AC waveform to a DC waveform. Schottky diodes have the added advantage over conventional PN junction diodes in that they work well at high frequency. The diodes used for BBU studies were manufactured by Herotek (model DZM124NB) and work across a frequency range from 10 MHz to 12.4 GHz [78]. 114

FIG. 5.1: Successive frames in time (progressing from left to right) from a movie of the<br />

synchrotron light monitor in the second endloop at the onset of BBU.<br />

5.1 Overview<br />

While the remainder of this chapter is dedicated to describing the details of<br />

the quantitative measurements, Fig. 5.1 illustrates a qualitative characterization of<br />

BBU. Figure 5.1 shows a series of frames from a recording of a synchrotron light<br />

monitor located in the second recirculation arc of the FEL Driver. During the<br />

recording, the average beam current was being slowly increased until beam breakup<br />

developed. The instability clearly manifests itself as vertical growth which continues<br />

until beam losses become large enough to trip the machine off. The time elapsed<br />

from the first to the last frame of Fig. 5.1 is approximately 0.25 s.<br />

From the point of view of a machine operator in the control room, the only<br />

indication that the operating current is approaching the threshold current are obser-<br />

vations of the SLM image growing as depicted in Fig. 5.1. Additional characteristics<br />

of the presence of BBU - from an operator’s perspective - are single, hard machine<br />

trips at one particular beam loss monitor (BLM) location. In most instances, these<br />

BLM trips occurred in the 5F region of the Driver where the recirculated beam is<br />

re-injected through the linac and the beam envelopes are largest.<br />

Clearly a more quantitative method is needed to confirm that a machine trip<br />

is due to BBU. Additional measurements are required to ascertain which cavity<br />

contains the dangerous HOM and to determine the frequency of the mode. Fur-<br />

113<br />

thermore, adequately benchmarking BBU codes requires accurately measuring the

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