Beam Condition Monitors and a Luminometer Based on Diamond Sensors

Similar documents
Diamond sensors as beam conditions monitors in CMS and LHC

Use of Single Crystal Diamond for the Fast Beam Conditions Monitor and the Pixel Luminosity Tracker for CMS at the LHC

Upgrade of the CMS Instrumentation for luminosity and machine induced background measurements

CMS Tracker Upgrades. R&D Plans, Present Status and Perspectives. Benedikt Vormwald Hamburg University on behalf of the CMS collaboration

The CMS electromagnetic calorimeter barrel upgrade for High-Luminosity LHC

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

Phase 1 upgrade of the CMS pixel detector

Upgrade of the CMS Tracker for the High Luminosity LHC

Installation, Commissioning and Performance of the CMS Electromagnetic Calorimeter (ECAL) Electronics

Operational Experience with the ATLAS Pixel Detector

The CMS Outer HCAL SiPM Upgrade.

Test Beam Measurements for the Upgrade of the CMS Phase I Pixel Detector

The LHCb Upgrade BEACH Simon Akar on behalf of the LHCb collaboration

1. PUBLISHABLE SUMMARY

CALICE AHCAL overview

KLauS4: A Multi-Channel SiPM Charge Readout ASIC in 0.18 µm UMC CMOS Technology

Firmware development and testing of the ATLAS IBL Read-Out Driver card

ATLAS Tracker and Pixel Operational Experience

Construction and first beam-tests of silicon-tungsten prototype modules for the CMS High Granularity Calorimeter for HL-LHC

A High-Granularity Timing Detector for the Phase-II upgrade of the ATLAS Detector system

A new strips tracker for the upgraded ATLAS ITk detector

PoS(EPS-HEP2017)476. The CMS Tracker upgrade for HL-LHC. Sudha Ahuja on behalf of the CMS Collaboration

What do the experiments want?

ATLAS ITk and new pixel sensors technologies

The LHCb VELO Upgrade

Upgrade of the ATLAS Thin Gap Chamber Electronics for HL-LHC. Yasuyuki Horii, Nagoya University, on Behalf of the ATLAS Muon Collaboration

Readout electronics for LumiCal detector

ATLAS Muon Trigger and Readout Considerations. Yasuyuki Horii Nagoya University on Behalf of the ATLAS Muon Collaboration

The CMS Silicon Strip Tracker and its Electronic Readout

MuLan Experiment Progress Report

The Run-2 ATLAS. ATLAS Trigger System: Design, Performance and Plans

A 130nm CMOS Evaluation Digitizer Chip for Silicon Strips readout at the ILC

The CMS Pixel Detector Phase-1 Upgrade

Status of SVT front-end electronics M. Citterio on behalf of INFN and University of Milan

PoS(LHCP2018)031. ATLAS Forward Proton Detector

Track Triggers for ATLAS

Pixel characterization for the ITS/MFT upgrade. Audrey Francisco

ATLAS strip detector upgrade for the HL-LHC

Traditional analog QDC chain and Digital Pulse Processing [1]

Streaming Readout for EIC Experiments

Preparing for the Future: Upgrades of the CMS Pixel Detector

A Prototype Amplifier-Discriminator Chip for the GLAST Silicon-Strip Tracker

Plans for RPC DHCAL Prototype. David Underwood Argonne National Laboratory

arxiv: v1 [physics.ins-det] 5 Sep 2011

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

Beam Conditions Monitors for the CMS experiment at the LHC

MAROC: Multi-Anode ReadOut Chip for MaPMTs

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

Design and Test of a 65nm CMOS Front-End with Zero Dead Time for Next Generation Pixel Detectors

Development of Telescope Readout System based on FELIX for Testbeam Experiments

A High Granularity Timing Detector for the Phase II Upgrade of the ATLAS experiment

Chapter 4 Vertex. Qun Ouyang. Nov.10 th, 2017Beijing. CEPC detector CDR mini-review

Contents. The AMADEUS experiment at the DAFNE collider. The AMADEUS trigger. SiPM characterization and lab tests

Data acquisition and Trigger (with emphasis on LHC)

Front-End Electronics and Feature-Extraction Algorithm for the PANDA Electromagnetic Calorimeter

Wolfgang Lohmann, BTU and DESY

PMF the front end electronic for the ALFA detector

The Commissioning of the ATLAS Pixel Detector

Totem Experiment Status Report

LHCb Preshower(PS) and Scintillating Pad Detector (SPD): commissioning, calibration, and monitoring

The DMILL readout chip for the CMS pixel detector

Data acquisition and Trigger (with emphasis on LHC)

SPD VERY FRONT END ELECTRONICS


Pixel sensors with different pitch layouts for ATLAS Phase-II upgrade

Micromegas calorimetry R&D

Strip Detectors. Principal: Silicon strip detector. Ingrid--MariaGregor,SemiconductorsasParticleDetectors. metallization (Al) p +--strips

The CMS ECAL Laser Monitoring System

Study of the ALICE Time of Flight Readout System - AFRO

A High-Granularity Timing Detector for the Phase-II upgrade of the ATLAS Calorimeter system Detector concept description and first beam test results

The CMS ECAL Laser Monitoring System

Layout and prototyping of the new ATLAS Inner Tracker for the High Luminosity LHC

ATLAS LAr Electronics Optimization and Studies of High-Granularity Forward Calorimetry

Towards an ADC for the Liquid Argon Electronics Upgrade

Design of the Front-End Readout Electronics for ATLAS Tile Calorimeter at the slhc

R D 5 3 R D 5 3. Recent Progress of RD53 Collaboration towards next generation Pixel ROC for HL_LHC

Development of a Highly Selective First-Level Muon Trigger for ATLAS at HL-LHC Exploiting Precision Muon Drift-Tube Data

Development of Pixel Detectors for the Inner Tracker Upgrade of the ATLAS Experiment

arxiv:physics/ v1 [physics.ins-det] 19 Oct 2001

The Architecture of the BTeV Pixel Readout Chip

arxiv: v2 [physics.ins-det] 24 Oct 2012

D. Ferrère, Université de Genève on behalf of the ATLAS collaboration

PoS(Vertex 2016)071. The LHCb VELO for Phase 1 Upgrade. Cameron Dean, on behalf of the LHCb Collaboration

Data Compression and Analysis Methods for High- Throughput Radiation Detector Systems

Progress towards a 256 channel multianode microchannel plate photomultiplier system with picosecond timing

CMS Conference Report

Data Acquisition System for the Angra Project

A Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers

Status of Front End Development

Short-Strip ASIC (SSA): A 65nm Silicon-Strip Readout ASIC for the Pixel-Strip (PS) Module of the CMS Outer Tracker Detector Upgrade at HL-LHC

Front-End electronics developments for CALICE W-Si calorimeter

Calorimetry in particle physics experiments

AIDA-2020 Advanced European Infrastructures for Detectors at Accelerators. Milestone Report

Performance of 8-stage Multianode Photomultipliers

Development of the FVTX trigger

The VELO Upgrade. Eddy Jans, a (on behalf of the LHCb VELO Upgrade group) a

Hardware Trigger Processor for the MDT System

Calorimeter Monitoring at DØ

Data acquisi*on and Trigger - Trigger -

A tracking detector to study O(1 GeV) ν μ CC interactions

Transcription:

Beam Condition Monitors and a Luminometer Based on Diamond Sensors Wolfgang Lange, DESY Zeuthen and CMS BRIL group Beam Condition Monitors and a Luminometer Based on Diamond Sensors INSTR14 in Novosibirsk, February 25 2014

Outline Introduction Beam Condition Monitors, CMS BCM1F before the current shutdown System design, performance, limitations Upgrade in current shutdown Description, design, beam test results Conclusions Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 2

Beam Condition Monitor Context LHC running at unprecedented beam energies and intensities Even small beam losses may cause damage to CMS detector components Purpose of Beam Condition Monitors CMS Monitor particle fluxes near the beam pipe Ensure sufficiently low inner detector occupancy for data-taking Detect beam loss conditions Initiate reactions when necessary (beam abort) Uses different beam condition monitors in its BRM system Integrating monitors (signal current)! BCM1L, BCM2 Bunch by bunch monitors! scintillators and BCM1F Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 3

Fast Beam Condition Monitor BCM1F (up to 2012) Module LHC CMS 8 5mm x 5mm single-crystal CVD diamonds (Element 6) positioned around the beam-pipe, radial distance 4.5 cm, 1.8 m from interaction point Diamond! no cooling, robust, radiation-hard Sensor module: diamond, radiation-hard preamplifier, optical driver Bunch-by-bunch information on flux of beam halo and collision products Monitor condition of beam: ensure low radiation for silicon tracker Calculate luminosity Readout independent of CMS DAQ Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 4

BCM1F Electronics (up to 2012) Output: analog spectra ADC! monitoring hit rates Discriminator! Look-up table LUT Recording Histogram Unit RHU Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 5

What can be seen with such a device? Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 6

Performance of BCM1F (up to 2012) - 1 - Operated right from the start of LHC! first (splash) beam in LHC already seen - measures underground rates and time structure of beams - discovery of Albedo Effect (afterglow of slow particles) - delivers relevant background rates to CMS and to LHC control room - measures online luminosity Bunch structure inside LHC, abort gap on the right Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 7

Performance of BCM1F (up to 2012) - 2 - Operated right from the start of LHC: first (splash) beam in LHC seen - measures underground rates and time structure of beams - discovery of Albedo Effect (afterglow of slow particles) - delivers relevant background rates to CMS and to LHC control room - measures online luminosity Life Cycle of a fill in the LHC Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 8

Performance of BCM1F (up to 2012) - 3 - Operated right from the start of LHC: first (splash) beam in LHC seen - measures underground rates and time structure of beams - discovery of Albedo Effect (afterglow of slow particles) - delivers relevant background rates to CMS and to LHC control room - measures online luminosity Albedo Effect after collisions: excitation of material slow remaining particles lifetime ~2 "s Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 9

Performance of BCM1F (up to 2012) - 4 - Operated right from the start of LHC: first (splash) beam in LHC seen - measures underground rates and time structure of beams - discovery of Albedo Effect (afterglow of slow particles) - delivers relevant background rates to CMS and to LHC control room - measures online luminosity Collision rates (LUT) are used for luminosity measurements: Requires calibration online luminosity in CMS done by Hadron Forward Calorimeter (HF) Test of BCM1F as online luminometer: good agreement validated with calculations of HF, pixels! has potential as online luminometer advantage: decoupled from CMS DAQ Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 10

Limitations of BCM1F (up to 2012) - preamp has 25 ns shaping time to slow for 25 ns bunch spacing - preamp needs a long recovery time from large input signals (overdriven, saturated) - laser diodes (analog signal transmission) have radiation damage - diamond sensors show radiation damage! polarization! how to cure? - only 4 sensors on each side of the interaction point! saturation / pile-up problems Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 11

Upgrade Program of BCM1F in the current Shutdown - preamp has 25 ns shaping time to slow for 25 ns bunch spacing - preamp needs a long recovery time from large input signals (overdriven, saturated) - laser diodes (analog signal transmission) have radiation damage - diamond sensors show radiation damage! polarization! how to cure? - only 4 sensors on each side of the interaction point! saturation / pile-up problems Design of a new preamp: rise time below 12 ns fast recovery from overdrive differential outputs use of components with extended high voltage tolerance Moving of laser diodes to a less exposed area Adding slow control for current and gain (compensation metallization of sensors split into two pads use of 12 sensors with two pads each! 24 channels per side Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 12

Upgrade Program of BCM1F in the current Shutdown - preamp has 25 ns shaping time to slow for 25 ns bunch spacing - preamp needs a long recovery time from large input signals (overdriven, saturated) - laser diodes (analog signal transmission) have radiation damage - diamond sensors show radiation damage! polarization! how to cure? - only 4 sensors on each side of the interaction point! saturation / pile-up problems Design of a new preamp: rise time below 12 ns fast recovery from overdrive differential outputs use of components with extended high voltage tolerance Moving of laser diodes to a less exposed area Adding slow control for current and gain (compensation metallization of sensors split into two pads use of 12 sensors with two pads each! 24 channels per side Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 13

Upgrade Program of BCM1F in the current Shutdown - preamp has 25 ns shaping time to slow for 25 ns bunch spacing - preamp needs a long recovery time from large input signals (overdriven, saturated) - laser diodes (analog signal transmission) have radiation damage - diamond sensors show radiation damage! polarization! how to cure? - only 4 sensors on each side of the interaction point! saturation / pile-up problems Design of a new preamp: rise time below 12 ns fast recovery from overdrive differential outputs use of components with extended high voltage tolerance Moving of laser diodes to a less exposed area Adding slow control for current and gain (compensation metallization of sensors split into two pads use of 12 sensors with two pads each! 24 channels per side Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 14

Upgrade Program of BCM1F in the current Shutdown - preamp has 25 ns shaping time to slow for 25 ns bunch spacing - preamp needs a long recovery time from large input signals (overdriven, saturated) - laser diodes (analog signal transmission) have radiation damage - diamond sensors show radiation damage! polarization! how to cure? - only 4 sensors on each side of the interaction point! saturation / pile-up problems Design of a new preamp: rise time below 12 ns fast recovery from overdrive differential outputs use of components with extended high voltage tolerance Moving of laser diodes to a less exposed area Adding slow control for current and gain (compensation metallization of sensors split into two pads use of 12 sensors with two pads each! 24 channels per side Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 15

Upgrade Program of BCM1F in the current Shutdown Implications of LHC upgrade for BCM1F Radiation: Luminosity 10 34 cm -2 s -1! BCM1F expects charged particle flux ~3x10 7 cm -2 s -1 25 ns bunch spacing High hit rate 12 diamonds with 2 pads per diamond, both sides of IP! 48 channels Minimize and deal with radiation damage Scale up full system from 8 channels Faster electronics (preamp) Integrate readout with other luminosity subsystems Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 16

From Plans to Reality: the re-designed carriage The C-shape carries sensors and preamps. All wiring and support will be located on a one-piece-rigid-flexible PCB (Printed Circuit Board) Laser drivers go further away (r, z). Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 17

From Plans to Reality: the re-designed frontend chip ASIC designed by AGH Krakow (PL), Designer: Dominik Przyborowski IBM CMOS-8RF-130nm technology (radiation hard, submitted via CERN) ~50 mv/fc charge gain < 1k electrons ENC Sophisticated calibration logic 4 channels on 1 chip Laboratory measurements of the full readout chain of upgraded BCM1F Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 18

From Plans to Reality: improving the optical chain Radiation damage of laser driver visible in decreasing signal amplitude: 25% gain lost in BCM1F optical transmission after 30 fb -1 Countermeasures: Go away from the hot area Compensate the loss in gain compensate for the shifted laser threshold Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 19

Upgrade of Backend Electronics Use tried and true discriminator path for initial running while commissioning digitizer path! following slide LUT: create coincidences between all 48 channels! patterns RHU for readout (later slide)! dedicated histograms Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 20

Signal Processing Two parallel tracks to be followed: Discriminators Fixed-threshold vs. constant-fraction Digitizer with fast peak-finding algorithms Constant-fraction: better time resolution Fixed-threshold: lower deadtime Preliminary conclusion: deadtime outweighs resolution -> use FTD (CAEN V895) for primary path but install CFD to run and test in parallel Identify pulse arrival time and peak height, distinguish signals close in time (overlapping) deconvolution Development of algorithms ongoing Current hardware choice: utca ADC FMC mezzanine system. Multiple FMC candidates, to be tested Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 21

Recording Histogram Unit (RHU) RHU: Readout of full-orbit histograms No deadtime (buffered readout) 8 histogramming input channels Bins of 6.25 ns = 4/bunch bucket (14k bins/orbit) Bunch clock, orbit clock, beam abort Configurable sampling period Ethernet readout Developed at DESY-Zeuthen Prototype installed Sept. 2012, validated during 2012-2013 run Very flexible unit (FPGA based, own interface and OS) Physics friendly data compression for direct access Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 22

Conclusions and Outlook Many improvements in the works to increase effectiveness Carriage: 48 channels, single PCB Diamond sensors: minimize effects of radiation damage using higher voltage New fast front end ASIC to reduce inefficiencies Optical chain: lower radiation for laser driver, multi-amplitude test pulses Back end: Discriminator path in parallel with digitizer peak-finding RHU for collection of hit rates Algorithms for luminosity measurement Outlook Installation of 4 carriages (full system) planned begin of September Comissioning of all subsystems soon after installation and recovery of the LHC Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 23

What should I add? Thank you for your attention!!"#$%&' (# )*%+#*%,! Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 24

Backup Slides (1) - Very first beam in LHC Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 25

Backup Slides (2) Luminosity Basics Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 26

Backup Slides (3) Discriminators Current discriminator: CAEN v258b fixed-threshold discriminator - Does not discriminate pulses closer than ~12 ns: deadtime causes loss of consecutive signals - Triggers pulses of different amplitudes at different times: time walk #T ~12 ns Meanwhile tested: two constant-fraction discriminators: CAEN V812, PSI CFD950 Both CFDs significantly improve on FTD time walk - V812: better time resolution for trigger of single pulse - CFD950: better resolution between consecutive pulses Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 27

Backup Slides (4) upgraded frontend ASIC Wolfgang Lange BCM with Diamonds 25-Feb-2014 Page 28