Beam Secondary Shower Acquisition System: First Beam Profile Measurements with QIE10 Front-End BE-BI-BL Jose Luis Sirvent Blasco 2 Jose Luis Sirvent Blasco PhD. Student Emittance Meeting 03/11/2015

0. Motivation 0.1 Beam Secondary shower acquisition system upgrade. Current System: Need to set-up working point of PMT gain & Filter selection Working point has an impact on Beam sigma measurements (PMT Saturation) Limited dynamic range in any configuration (Tails measurements) High Intensity beams rise up noise level. Upgraded System: New detector: pCVD Diamond detectors Tunnel acquisitions and digital data transmission GBT protocol: Avoid long coax cabling High dynamic range (1e6) no tuneable parameters : Several channels on parallel or Logarithmic acquisitions BE-BI-BL Jose Luis Sirvent Blasco 3 Scintillator Filters PMT Preamplifiers

1. Set-up (BA5) 1.1 Tunnel Scheme with dual pCVD diamond Detector BE-BI-BL Jose Luis Sirvent Blasco 4 Connections: A  5V (9V) A  +12V A  -12V A  HV A  Signal TOP A  Signal BOTTOM Front-End Channels: CH1  TOP CH2  BOTTOM ~ 1.6 m

BE-BI-BL Jose Luis Sirvent Blasco 5 1. Set-up (BA5) 1.1 Tunnel Scheme with dual pCVD diamond Detector

BE-BI-BL Jose Luis Sirvent Blasco 6 1. Set-up (BA5) 1.2 Installation performed on technical Stop 02/09/2015 pCVD DD_1 pCVD DD_2 TI. Amplif To Surface (~80m) CK50 CB50 CBH50SMF Beam Pipe HV -12V +12V Sig_1 Igloo2 Dev. Kit GBT Core SDRAM Storage PC Communication Power Supply Instrumentation Sig_2 Digital Front-End Prototype Power (FEASTMP) QIE10 Mezzanine VTRx Igloo2_Umd Mezzanine Board (from CMS ngCCM) Bi-directional GBT optical 4.8Gbps (Data transfer, Synchronization & Control) Scope pCVD DD_1 pCVD DD_2 CB50 +10V

BE-BI-BL Jose Luis Sirvent Blasco 7 1. Set-up (BA5) 1.3 Surface Scheme for pCVD Analog & Digital Readout Igloo2 Dev. Kit SI5338 EVB PLL + Jitter Cleaner Trigger + Turn Clock Conditioning Circuit VTRx B.CLK 40MHz

2. Measurements 2.1 First Losses detected on the tree systems BE-BI-BL Jose Luis Sirvent Blasco 8 Observations: 1. Signals from the pCVD diamond detectors show very fast single losses 2. Detector size seems to be important for losses detection (random nature) 3. Top detector is showing a lower amplitude for some reason (same set-up) 4. Losses correlation with PMT only on very high losses.

3.Measurement Campaign #1: 2015_10_09 (Night 21:14) SPS BWS51731 H & V BE-BI-BL Jose Luis Sirvent Blasco 9 Beam Test Conditions: 1.LHC_Pilot/MD2 1e11 26GeV Tests objectives: Beam profile measurement efficiency of pCVDs VS Scintillators for this specific beam. Statistics Study

BE-BI-BL Jose Luis Sirvent Blasco 10 3.Measurement Campaign #1: 2015_10_09 BWS517-H 21:20:48 (Night # 0) LHC_Pilot 1e11 26GeV

BE-BI-BL Jose Luis Sirvent Blasco 11 3.Measurement Campaign #1 : 2015_10_09 BWS517-H 21:33:05 (Night # 1) LHC_Pilot 1e11 26GeV

BE-BI-BL Jose Luis Sirvent Blasco 12 3.Measurement Campaign #1 : 2015_10_09 (Summary) LHC_Pilot/MD2 26GeV MorningNight (Beam dynamics changed profile width) Datasets: 4 Beam profiles in each dataset, All signals taken with LeCroy Scope, Allways considering 1m/s, In & Out scans are mixed on these measurements (different speeds not considered). Conclusions: 1.Beam size calculated with both systems and beam sigma STD are comparable Clear from the Gaussian goodness-of-fit that for these beam conditions PMT and SCINT shows better performance. Very spicky profiles with diamond detectors: Detector effective area 1cm2 (pCVDs) VS 300cm2 (Scintillator) Particles distributed randomly in the shower cone Possibility of detecting with higher efficiency neutrons on pCVD diamonds than on Scintillator (to be checked) 2.Improvement shown when combining the diamonds measurements, but far from SCINT performance in goodness-of-fit.

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night 22:00h  2:30h) Beam Test Conditions: 1.LHC_Pilot/MD2 6.5e9 26GeV  No signal seen on pCVDs 2.LHC_Pilot/MD2 5.2e9 450GeV  Measurements shown 3.LHC_Pilot/MD2 1.1e11 450GeV  Measurements shown Tests objectives: Check beam profile measurement efficiency of pCVDs VS Scintillators at different beam intensities Test the QIE10 Front-end: Synchronization on triggering system Automatic calculation of acquisition delay QIE10 suitability for pCVD diamond detector readout QIE10 suitability for beam profile measurement (1% quantification error) Beam profile improvement with digital front-end.

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night #6) LHC_Pilot 5.2e9 PpB 450 GeV PMT Preamp close to saturation (non- linear region)!

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night #6) LHC_Pilot 5.2e9 PpB 450 GeV PMT Preamp close to saturation (non- linear region)! 1. Lower noise on tails (1) 2. Better SSE (2) 3. PMT Pre- amp close to saturation

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night #6) LHC_Pilot 5.2e9 PpB 450 GeV Not possible to compare sigma values: Wrong profile on PMT, preamp close to saturation

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night #6) LHC_Pilot 5.2e9 PpB 450 GeV First beam profiles with QIE10 Front-End on detail

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night #10) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night #10) LHC_Pilot 1.1e11 PpB 450 GeV 1. Much better profiles (1) 2. Comparable width (2) 3. Similar Performance (3)

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night #10) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night #10) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 2015_10_23 (Night #10) LHC_Pilot 1.1e11 PpB 450 GeV IN OUT

BE-BI-BL Jose Luis Sirvent Blasco Measurements Campaign #2: 4.1 Summary *Acknowledgements to E. Piselli and B. Dehning for his support and help during the measurements. Beam Intensity and Beam Energy influence on pCVD diamond detectors performance for beam profile monitoring. Diamonds on Surface VS QIE10 : better results obtained with QIE10 front-end in terms of noise and GOF. Need to optimize detectors placement based on Simulations for 26Gev and low intensity monitoring. For 1e11 PpB diamonds show comparable performance with the PMT + Scintillator system

BE-BI-BL Jose Luis Sirvent Blasco 24

Back-Up Slides BE-BI-BL Jose Luis Sirvent Blasco 25

BE-BI-BL Jose Luis Sirvent Blasco 26 Processing 2015_10_09 (Morning #11)

BE-BI-BL Jose Luis Sirvent Blasco 27 Processing 2015_10_09 (Morning #12)

BE-BI-BL Jose Luis Sirvent Blasco 28 Processing 2015_10_09 (Morning #13)

BE-BI-BL Jose Luis Sirvent Blasco 29 Processing 2015_10_09 BWS517-H 22:17:34 (Night # 4)

BE-BI-BL Jose Luis Sirvent Blasco 30 Processing 2015_10_09 BWS517-H 22:43:22 (Night # 5)

BE-BI-BL Jose Luis Sirvent Blasco 31 Processing 2015_10_09 BWS517-V 23:15:11 (Night # 6)

BE-BI-BL Jose Luis Sirvent Blasco 32 Processing 2015_10_09 BWS517-V 00:00:39 (Night # 8)

BE-BI-BL Jose Luis Sirvent Blasco 33 Processing 2015_10_09 BWS517-V 00:05:39 (Night # 9)

BE-BI-BL Jose Luis Sirvent Blasco 34 Processing 2015_10_09 BWS517-V 00:22:18 (Night # 10)

BE-BI-BL Jose Luis Sirvent Blasco 35 Processing 2015_10_09 BWS517-V (Night # 8)

BE-BI-BL Jose Luis Sirvent Blasco 36 Processing 2015_10_09 BWS517-V (Night # 8)

BE-BI-BL Jose Luis Sirvent Blasco 37 Processing 2015_10_09 BWS517-V (Night # 8)

BE-BI-BL Jose Luis Sirvent Blasco 38 Processing 2015_10_09 BWS517-V (Night # 8)

BE-BI-BL Jose Luis Sirvent Blasco 39

Processing BE-BI-BL Jose Luis Sirvent Blasco 40

BE-BI-BL Jose Luis Sirvent Blasco 41 Processing 2015_10_09 (Morning #12)

BE-BI-BL Jose Luis Sirvent Blasco 42 Processing 2015_10_09 (Morning #13)

2015_10_16 13:13:00 STFPRO1/ MD2 BE-BI-BL Jose Luis Sirvent Blasco 43

BE-BI-BL Jose Luis Sirvent Blasco 44 Processing 2015_10_23 (Night #7) LHC_Pilot 5.2e9 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 45 Processing 2015_10_23 (Night #7) LHC_Pilot 5.2e9 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 46 Processing 2015_10_23 (Night #7) LHC_Pilot 5.2e9 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 47 Processing 2015_10_23 (Night #7) LHC_Pilot 5.2e9 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 48 Processing 2015_10_23 (Night #8) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 49 Processing 2015_10_23 (Night #8) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 50 Processing 2015_10_23 (Night #8) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 51 Processing 2015_10_23 (Night #8) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 52 Processing 2015_10_23 (Night #11) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 53 Processing 2015_10_23 (Night #11) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 54 Processing 2015_10_23 (Night #11) LHC_Pilot 1.1e11 PpB 450 GeV

BE-BI-BL Jose Luis Sirvent Blasco 55 Processing 2015_10_23 (Night #11) LHC_Pilot 1.1e11 PpB 450 GeV