TY - GEN
T1 - A GAS-JET profile monitor for the CLIC drive beam
AU - Jeff, A.
AU - Holzer, E. B.
AU - Lefèvre, T.
AU - Tzoganis, V.
AU - Welsch, C. P.
N1 - Publisher Copyright:
Copyright © 2013 by JACoW.
PY - 2013/12/1
Y1 - 2013/12/1
N2 - The Compact Linear Collider (CLIC) will use a novel acceleration scheme in which energy extracted from a very intense beam of relatively low-energy electrons (the Drive Beam) is used to accelerate a lower intensity Main Beam to very high energy. The high intensity of the Drive Beam, with pulses of more than 1015 electrons, poses a challenge for conventional profile measurements such as wire scanners. Thus, new non-invasive profile measurements are being investigated. Profile monitors using gas ionisation or fluorescence have been used at a number of accelerators. Typically, extra gas must be injected at the monitor and the rise in pressure spreads for some distance down the beam pipe. In contrast, a gas jet can be fired across the beam into a receiving chamber, with little gas escaping into the rest of the beam pipe. In addition, a gas jet shaped into a thin plane can be used like a screen on which the beam cross-section is imaged. In this paper we present some arrangements for the generation of such a jet. In addition to jet shaping using nozzles and skimmers, we propose a new scheme to use matter-wave interference with a Fresnel Zone Plate to bring an atomic jet to a narrow focus.
AB - The Compact Linear Collider (CLIC) will use a novel acceleration scheme in which energy extracted from a very intense beam of relatively low-energy electrons (the Drive Beam) is used to accelerate a lower intensity Main Beam to very high energy. The high intensity of the Drive Beam, with pulses of more than 1015 electrons, poses a challenge for conventional profile measurements such as wire scanners. Thus, new non-invasive profile measurements are being investigated. Profile monitors using gas ionisation or fluorescence have been used at a number of accelerators. Typically, extra gas must be injected at the monitor and the rise in pressure spreads for some distance down the beam pipe. In contrast, a gas jet can be fired across the beam into a receiving chamber, with little gas escaping into the rest of the beam pipe. In addition, a gas jet shaped into a thin plane can be used like a screen on which the beam cross-section is imaged. In this paper we present some arrangements for the generation of such a jet. In addition to jet shaping using nozzles and skimmers, we propose a new scheme to use matter-wave interference with a Fresnel Zone Plate to bring an atomic jet to a narrow focus.
UR - http://www.scopus.com/inward/record.url?scp=84920545387&partnerID=8YFLogxK
M3 - Conference contribution
AN - SCOPUS:84920545387
T3 - IBIC 2013: Proceedings of the 2nd International Beam Instrumentation Conference
SP - 224
EP - 227
BT - IBIC 2013
PB - Joint Accelerator Conferences Website (JACoW)
T2 - 2nd International Beam Instrumentation Conference, IBIC 2013
Y2 - 16 September 2013 through 19 September 2013
ER -