1. 1 Proposal for a Multi-Optical Transition Radiation System in ATF2 A. Faus-Golfe, D. McCormick IFIC – SLAC 11 June 2009 8 th TB/SGC Meeting

2. 2 Motivation and Objectives - We propose to install a series of four Optical Transition Radiation (OTR) monitors in the beam diagnostic section of the EXT line of ATF, close to the multi wire scanner system. -The system would be a valuable tool for measuring beam sizes and emittances from the ATF DR. - An original OTR design demonstrated the ability to measure a 5.5 um beam size in one beam pulse and to take many fast measurement.

3. 3 PROPOSAL: Multi OTR System (4 units) (collaboration involving SLAC and IFIC, with the KEK support): beam dynamics studies, design, construction, and characterization including associated electronics - Horizontal and vertical beam size measurement in one beam pulse with 2 um resolution - OTR’s placed close to the wire scanners: definitive test of OTR as emittance diagnostic device. New Multi-OTR System In the diagnostic section of the ATF EXT line 5 wire scanners are located to allow emittance measurements (with 10 um tungsten and 7 um carbon wires) - Requires many machine pulses, slow measurements - Resolution: less than 2 um in X and 0.3 um in Y

4. 4 New design of the OTR for ATF-ATF2 Existing OTR monitor (OTR1X) 4 The OTR1X monitor is installed in the ATF2 EXT line after the septum magnets. It has been used to study the relation between the beam trajectory and the emittance growth due to non-linear fields in the extraction process open the bump in DR and EXT close the bump in the DR OTR monitor Measured beam sizes on 19 th Dec’07 CCD camera Inferred emittances from modeled ß-functions and dispersions

5. 5 New design of the OTR for ATF-ATF2 Current OTR setup Current OTR installed in the ATF EXT line target CCD camera Space required for current OTR The OTR1X was an evolved design rather than a optimized one. –New parts were added to the existing OTR to add functionality. Instead of making new design they were added bit by bit. As a result the OTR1X is a patchwork of parts and takes up a lot of beam line space. Existing OTR targets were rather thick, about 0.5mm of copper, beryllium or glassy carbon. This caused radiation darkening of the glass lens and camera damage. The camera CCD was not parallel to the target. This meant that the beam spot was in focus on only a small portion of the target. If the beam moved, the image had to be refocused.

6. 6 - Target actuator relocated to the top (no interference with the girder) and smaller design  greater flexibility in the OTR placement - Thinner target  reduce lens radiation darkening - CCD camera parallel to the target. This will put the entire target into focus and reduce the need to adjust focus during normal operation  greater depth of field. - 12 bit camera for more dynamic range with smaller pixel size for more resolution. - The extreme thinness of the aluminum’s 1200 Angstroms will reduce the power deposition in the aluminum and coupled to larger beam spot sizes should eliminate target damage problems. New OTRs will have same controls and motion capabilities as current OTR with the following improvements: New OTR monitor design

7. 7 Optics and location for the new OTR’s

8. 8 MAD Twiss parameters and beam size calculations for OTR1X and MW0X- MW4X of the ATF EXT line optics (V4.1) OTR1X_ old Start EXT OTR1XMW0XMW1XMW2XMW3XMW4X  x [nm.rad] 2.0  y [pm.rad] 12 EE 8.00 x10 -4  x [m] 8.2676.8537.3923.28212.1223.82411.4123.758  y [m] 5.2272.9415.6179.2714.49613.7903.5279.702 D x [m]0.3890.0000.4360.000 D y [m]0.000  x [2  ] 0.1140.0000.1222.8752.9052.9833.1033.184  x [2  ] 0.0002.7520.0300.0780.1200.080  y [2  ] 0.3560.00000.3662.1422.1842.2512.3632.455  y [2  ] 0.00001.7750.0420.0670.1120.092  x [  m] 439.78117.07470.1081.02155.7187.45151.0886.69  y [  m] 7.855.898.1410.467.2812.756.4510.70 The four OTR’s have to be as close as possible to the wire scanners in order to have similar conditions.

9. 9 Optics and location for the new OTR’s Input parameters: 50.000 particles x, y and E gaussian distribution Beam sizes, ß-functions and emittances for OTR1X and MW0X-MW4X of the ATF EXT line optics calculated from tracking simulations using PLACET and MAD programs. OTR1X_ old OTR1XMW0XMW1XMW2XMW3XMW4X  x [  m] 337.41370.3981.73157.0688.00151.3186.87  y [  m] 7.248.1310.577.3612.836.4410.69  x [nm.rad] 2.02  y [pm.rad] 1.18 1.19  x [m] 3.30512.2123.83411.1313.735  y [m] 4.4355.5889.3984.55113.8413.4849.603 Spot sizes estimated for the new OTR locations are a bit larger than the spots that damaged the cooper target in the original OTR tests  no target damage expected

10. 10 Beam plots y vs x x’ vs xy’ vs y OTR1X MW0X MW1X

11. 11 Beam plots x’ vs x MW2X MW3X MW4X y vs x y’ vs y

12. 12 Proposed locations for the new OTR’s In order to make the validation tests of the OTR as a beam emittance diagnostic device, the proposed locations of the four OTR’s are as close as possible to the five wire scanners. A length of about 300 mm will be needed for each OTR unit.

13. 13 Proposed locations for the new OTR’s

14. 14 Proposed locations for the new OTR’s

15. 15 Proposed locations for the new OTR’s

16. 16 Proposed locations for the new OTR’s

17. 17 Manpower The team is a collaborative effort between the IFIC and SLAC. The people involved are: IFIC - A. Faus-Golfe, J. Alabau Gonzalvo, M. Alabau Pons, J. V. Civera Navarrete, C. Blanch Gutierrez and J. J. García Garrigós SLAC - D. McCormick, J. Nelson, B. McKee and J. Cruz

18. 18 Status and planning -The OTR design is essentially finished. - The first step will be the mechanical construction of the different parts and the procurement of the optical components, followed by the assembly and the calibration tests. - The system could be installed by the end of 2009 or later. - The commissioning could be done immediately after the units have been installed if there is beam time available for calibration.