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156 rue du Mont Rond Tel: +33 450 42 66 42 Espace Allondon Ouest Fax: +33 450 42 66 43 01630 Saint Genis Pouilly, France Email: info@bergoz.com Beam Loss Monitor User’s Manual Rev. 3.0 Japan U.S.A. Hayashi-Repic Co., Ltd. GMW Associates www.h-repic.co.jp ww.gmw.com sales@h-repic.co.jp sales@gmw.com China India...
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Record of updates Version Date Updates performed 06/2017 New release including BLM-DIF 03/2018 Review of the full manual. Obsoletes all previous versions...
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 2 INITIAL INSPECTION It is recommended that the shipment be inspected immediately upon delivery. If it is damaged in any way, contact Bergoz Instrumentation or your local distributor. The content of the shipment should be compared to the items listed on the invoice. Any discrepancy should be notified to Bergoz Instrumentation or its local distributor immediately. Unless promptly notified, Bergoz Instrumentation will not be responsible for such discrepancies. WARRANTY Bergoz Instrumentation warrants its beam current monitors to operate within specifications under normal use for a period of 12 months from the date of shipment. Spares, repairs and replacement parts are warranted for 90 days. Products not manufactured by Bergoz Instrumentation are covered solely by the warranty of the original manufacturer. In exercising this warranty, Bergoz Instrumentation will repair, or at its option, replace any product returned to Bergoz Instrumentation or its local distributor within the warranty period, provided that the warrantor's examination discloses that the product is defective due to workmanship or materials and that the defect has not been caused by misuse, neglect, accident or abnormal conditions or operations. Damages caused by ionizing radiations are specifically excluded from the warranty. Bergoz Instrumentation and its local distributors shall not be responsible for any consequential, incidental or special damages. ASSISTANCE Assistance in installation, use or calibration of Bergoz Instrumentation beam current monitors is available from Bergoz Instrumentation, 01630 Saint Genis Pouilly, France. It is recommended to send a detailed description of the problem by email to info@bergoz.com. SERVICE PROCEDURE Products requiring maintenance should be returned to Bergoz Instrumentation or its local distributor. Bergoz Instrumentation will repair or replace any product under warranty at no charge. The purchaser is only responsible for transportation charges. For products in need of repair after the warranty period, the customer must provide a purchase order before repairs can be initiated. Bergoz Instrumentation can issue fixed price quotations for most repairs. However, depending on the damage, it may be necessary to return the equipment to Bergoz Instrumentation to assess the cost of repair.
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 3 RETURN PROCEDURE All products returned for repair should include a detailed description of the defect or failure, name and fax number of the user. Contact Bergoz Instrumentation or your local distributor to determine where to return the product. Returns must be notified by fax prior to shipment. Return should be made prepaid. Bergoz Instrumentation will not accept freight-collect shipment. Shipment should be made via UPS, FedEx or DHL. Within Europe, the transportation service offered by the Post Offices "EMS" (Chronopost, Datapost, etc.) can be used. The delivery charges or customs clearance charges arising from the use of other carriers will be charged to the customer.
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 4 SCOPE OF USE Beam Loss Monitors based on PIN-photodiode signal coincidence detection can be used to evaluate beam loss of CW beam, long macropulses from synchrotrons, cyclotrons and high- repetition rate linacs. PIN-Photodiodes-based BLMs are of no use on beam with single pulses, e.g. laser-plasma accelerators, single bunch injection, low repetition rate linacs. Why? Because PIN-photodiode-based BLM outputs a single pulse whether it is hit by one secondary electron or 1000 such electrons and requires 100ns to recover before the next hit. Thus, it is not an integrating loss monitor. It relies on the statistical probability of being hit by secondary electrons. BLM MODELS Identify whether the model is BLM-SE, i.e. with unipolar single-ended output, or BLM-DIF, i.e. with differential 100-ohm output. Both models are equipped with two 7.34 mm2 BPW34 PIN-diodes. Note: BLM-XL with 150 mm2 S2662 is an older model no longer manufactured. Older denomination BLM-XS is now known as BLM-SE. QUICK CHECK You can check immediately that your BLM is working. To check the spurious count rate in each channel, this is what you need: • BLM-SE or BLM-DIF • Oscilloscope ≥100 MHz bandwidth • Power supplies: +5V, –5V, +24…25V • Resistor 4.7 kΩ ≥1/8W To check the actual count rate from secondary MIP electrons (minimum ionizing particles), a source decaying in beta- >900 keV is needed, e.g., Americium. These sources are not commonly available.
01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 5 Identify the connections Model BLM-SE HE10 Pin# ........ F unction 1 ............ G round 2 ............ + 5V 3 ............ n /c 4 ............ – 5V 5 ............ E nable/Disable B 6 ............ + 24…25V 7 .
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 7 OPERATING PRINCIPLE Detector Type The detector is sensitive to MIPs (minimum ionizing particles) produced when an accelerated particle hits the wall of the vacuum chamber. Refer to Annex I: “Electron Beam Loss Monitor” by W. Bialowons, F. Ridoutt and K. Wittenburg for the mechanism of beam loss in FODO structures due to accelerated particles scattering on residual gas molecules nuclei or vacuum chamber walls. The detector is composed of two PIN-diodes mounted face to face to form a 2-channel coincidence detector. +Bias Photon <100ns 100µm Coincidence +Bias Signal processing When an ionizing particle hits a PIN-diode, an electric charge is produced. A bias voltage allows collection of this charge. It is amplified to a level high enough for conventional logic. An AND-gate detects the coincidence of pulses from the two PIN-diodes. MIPs cause ionizations in both PIN-diodes, a coincidence occurs and an output pulse is generated. Photons do not cause ionization in both PIN-diodes. So, the coincidence circuit does not produce a pulse for photons. The amplification gain of each channel is adjusted with a potentiometer. Efficiency of the detector Overall, MIPs are detected with an efficiency > 30 %. See Annex III: “Radiation Resistance of Beam Loss Monitor” by K. Wehrheim and K. Wittenburg. The size of the PIN-diodes mounted on the circuit determines the detector’s solid angle. The coincidence scheme rejects very effectively the spurious noise from each channel to a figure well below 1 count/s. The channel gains can be adjusted to obtain negligible spurious count rates: < 0.1 count/min. See Annex II “A Beam Loss Monitor for HERA” by S. Schlögl and K. Wittenburg.
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 8 Dynamic range It is determined by the spurious noise of the detector and the maximum count rate. It exceeds 108. The spurious noise, in the absence of any background, is well below 1 count/s. In the presence of an intense X-ray background, the BLM must be shielded by 3 cm of lead to maintain the spurious count rate below 1 count/s. Without a lead shield, the spurious count rate has been observed on HERA to reach 100 counts/s. The detector recovers 100 ns after a hit, leading to 10 MHz maximum count rate. Radiation resistance Prototypes similar to production units were tested at DESY for radiation hardness. The unit under test was still working after 108 Rads dose (!). See Annex III: “Radiation Resistance of Beam Loss Monitor” by K. Wehrheim and K. Wittenburg. CALIBRATION BLM circuits are calibrated ex-factory for a spurious count rate of 10 kHz ±800 Hz. Discriminator readjustment on P1 and P2 is needed when the PIN-diodes are changed for another type (larger, smaller). Background count can be performed on line. On-the-bench verification / discriminator readjustment To adjust the spurious count rate, power up the BLM. Connect a frequency counter on the output. When measuring BLM-DIF output, either Out+ or Out– can be monitored. To readjust channel A, apply +5V via a 4.7kΩ resistor to “Enable/Disable B”. Adjust potentiometer P1 till 9.6~10.4 kHz output. To calibrate channel B, apply +5V via a 4.7kΩ resistor to “Enable/Disable A”. Adjust potentiometer P2 till 9.6~10.4 kHz output. On-line check Apply ≥ +1V alternately to Enable/Disable A and Enable/Disable B. Observe the count rate to be in range 9.6~10.4 kHz. Enable/Disable A resp. Enable/Disable B draws 120 µA from +1 V.
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 9 CHANGING THE PIN-PHOTODIODES PIN-photodiodes can be changed by the user for a larger-area model. Two similar diodes per BLM are required. Instructions • Make sure the BLM works properly before modification: See QUICK CHECK, in this manual. • Remove the printed circuit from its enclosure: • BLM-SE: Pull gently on the copper shield, the PCB is glued to the bucket. • BLM-DIF: Remove the (4) screws off the bakelite box bottom. • Desolder the copper shield and remove it. • Desolder the PIN-diodes and remove them. • Install the new PIN-diodes. They should be facing each other. Their active areas should overlap each other.! Beware of the PIN diodes polarity. There are two possible configurations with the correct polarity: Note the common cathodes WARNING: Installing PIN-diodes with the wrong polarity voids the warranty. • Execute a QUICK CHECK before the copper shield is re-soldered. • Re-solder the copper shield. Make sure the copper shield does not touch the PIN-diodes leads! If needed, use polyvinyl adhesive tape to isolate the inside of the shield. • Re-adjust the BLM discriminator levels P1 and P3. See CALIBRATION in this manual. • Please note: large area PIN-photodiodes have more dark current, so the span of P1 and P2...
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 10 COMPTON ELECTRONS SHIELD Production of Compton electrons in the BLM PIN-photodiodes has been observed on very- high energy leptons accelerators (HERA-e, LEP). The consequence of Compton electrons production in one PIN-photodiode is that it may cause ionization in the other PIN-diode. As a result, the PIN-photodiodes produce pulses which are coincident and the BLM gives an output pulse. On very high energy leptons accelerators, these Compton electrons increase the background noise significantly The increase in background noise reduces the BLM useful dynamic range. A way to avoid this problem was sought. It was proposed to install a shield between the two PIN-photodiodes. This proposed improvement was successfully tested at both LEP and HERA: It reduces the Compton electron-induced noise significantly. The shield is made out of 200 µm thick copper foil. It is grounded via a high value resistor to prevent static charge build-up. Improvement in the useful dynamic range of the LEP Beam Loss Monitor, T.Spickermann, CERN, and K.Wittenburg, DESY, to be published...
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 11 INSTALLATION Mechanical mounting The BLM must be oriented facing the particles to be detected: Detector front BEAM LOSS MONITOR bergoz 2 4 6 8 10 1 3 5 7 9 Mathematical simulation would indicate where beam loss is most likely to occur (See Annex I for FODO structure beam loss). BLMs will generally be placed with the front applied against the magnets. BLM-SE can be screwed on brackets with two M3 screws. M3 screws will gently make their way into the Ø2.8mm holes of the ABS plastic. BLM-DIF features 4 mounting holes. Yet, it is preferable to attach the BLM with Velcro tape.
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 12 Mounting holes BLM-SE 33.5 mm 30 mm BLM-DIF 1.964 [49.89 mm]...
BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 13 BLM CONNECTIONS BLM-SE connects with a female HE10 connector e.g., 3M, type 3473-6000. Output with a 50-ohm coaxial cable connects to pin 10, ground on Pin 8. At DESY, RG-59 75-ohm coax cables are used for distances up to 100 meters without problems (K. Wittenburg, private communication, Febr. 9, 1995). For cables longer than 100 meters, a small amplifier is added in front of the scaler. BLM-DIF connects to an RJ45 plug. A recommended alternative is using Ethernet cable. Pair impedance is 100 ohms. Cat.5 or higher is recommended. It is not necessary that each pair is individually shielded because only one pair carries a pulsed signal. F/UTP aka FTP, S/UTP and SF/UTP are suitable. UTP must be avoided. STP is a generic name to describe S/UPT or SF-UTP. It is suitable. For long runs of cable, an overall shield and individual shielding of each pair is preferable for RFI rejection: S/FTP or F/FTP are recommended for long runs or high-noise areas. For acronyms, see: http://www.belden.com/blog/datacenters/STP-UTP-FTP-Cable-More-7-Types-When-to-Use- Them.cfm OUTPUT SIGNAL PROCESS Controls would use scalers with single-ended input or 100-ohm differential input. Laboratory tests can be made using a frequency counter. SPECIFICATIONS MIP detection efficiency > 30% PIN-photodiode surface 7,34 mm2 Spurious count rate < 0.1 Hz Up to 100Hz under 6e3 Grey/yr SR background < 1Hz under 6e3 Grey/yr SR background with 3cm lead shield Maximum count rate 10 MHz Enable/Disable A control ≥+1V, 120 µA...
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BERGOZ Instrumentation Beam Loss Monitor 01630 Saint Genis Pouilly, France Version 3.0 www.bergoz.com User’s Manual info@bergoz.com Page 14 ACKNOWLEDGMENTS The conceptual design of this Beam Loss Monitor is the work of several individuals at DESY- PKTR, over many years. I wish to thank them all here for their unique contribution to a very effective beam diagnostic tool, particularly Kay Wittenburg who has been the driving force all along. The contribution of Bergoz Instrumentation was to redesign the circuit. Surface mounted components allowed to make it smaller and more economical to assemble. Minor design changes were made. DESY granted Bergoz Instrumentation a license to use the original concept of the PIN- Photodiodes Beam Loss Monitor, to further develop it, to build and sell instruments based on this principle. Saint Genis Pouilly, last revised March 2018...
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