SLHC Radiation Test Results

Slides:



Advertisements
Similar presentations
AVANEX Livingston, Starlow Park, Livingston, EH54 8SF
Advertisements

The Radiation Tolerance of Specific Optical Fibers at −25 °C Joshua Abramovitch Southern Methodist University Faculty Advisors: Dr. Andy Liu, Dr. Jingbo.
Dror Malka and Zeev Zalevsky
S Digital Communication Systems Fiber-optic Communications - Supplementary.
1 William N MacPherson, Robert RJ Maier, James S Barton, Julian DC Jones Heriot-Watt University, EPS, Applied Optics and Photonics, Edinburgh, UK Alberto.
1 LIGHT EMISSION / DETECTION Lasers and LED Passive Elements Piotr Turowicz Poznan Supercomputing and Networking Center Training.
Detector lecturesT. Weidberg1 Opto-electronics Why use opto-electronics –General advantages –HEP experiments Elements of system –Emitters –Fibres –Receivers.
ATLAS/CMS Opto WG March '10 Tony Weidberg1 Radiation Damage Passive Components Versatile Link WP 2.3 –Todd Huffman, Mark Jones, Nick Ryder & Tony Weidberg.
PAGE 1 Glasgow 2014 Gary Stevens COMPACT DUAL CHANNEL OPTICAL FIBRE AMPLIFIER FOR SPACE COMMUNICATION APPLICATIONS G&H Systems and Technology Group & University.
L5 Optical Fiber Link and LAN Design
Fundamental of Fiber Optics. Optical Fiber Total Internal Reflection.
1 Fiber Optics FIBER PERFORMANCE. 2 Fiber Optics The purity of optical fiber is critical for the best transmission of an optical signal inside a fiber.
Data transmission needs and challenges for Frontier Particle Physics: Part 1 Why HEP needs special? Radiation-hard high speed optical links Lasers and.
*Supported by the EU FP7-PEOPLE-2012-ITN project nr , INFIERI, "Intelligent Fast Interconnected and Efficient Devices for Frontier Exploitation in.
LightABLE Production Status ID Week October 2014 Tony Weidberg1.
Optical Fiber Classification Can be classified in a number of ways On the basis of manufacturing Single component/Multi component Glass.
Light Wave Systems Dr Manoj Kumar Professor & Head Department of ECE DAVIET,Jalandhar.
Cryogenics for LCGT Technical Advisory Committee for LCGT ICRR SUZUKI, Toshikazu High Energy Accelerator Research Organization.
Overview of basic issues.   The design of the (Outer) Tracker Upgrade for phase 2 has been ongoing for more than 4 years  So far the (implicit) assumption.
ROSIER Ph End cap – TPC - LC DRAFT Definition of the front-end electronics and its cooling in the Alice TPC experiment Page 1A The Alice TPC.
Optical Links CERN Versatile Link Project VL – Oxford involvement CERN VL+ for ATLAS/CMS phase II upgrade – Introduction and aims – Oxford workpackage:
Optical absorption in commercial single mode optical fibers for the LHC machine T. Wijnands †, L.K. De Jonge †, J. Kuhnhenn ‡, S. K. Hoeffgen ‡, U. Weinand.
Evaluation of Multi-Gbps Optical Transceivers for Use in Future HEP Experiments Luis Amaral CERN – PH/ESE/BE – Opto 16/09/2008.
SLHC Proposal B Status Optical Readout System Irradiation Guidelines K.K. Gan, Karl Gill, Jan Troska, Francois Vasey, Todd Huffman, Cigdem Issever, Tony.
Commissioning and Operation of the CMS Tracker analogue optical link system at TIF with CMSSW: R.Bainbridge, A.Dos Santos Assis Jesus, K.A.Gill, V. Radicci.
Tony WeidbergATLAS/CMS Opto WG March '111 Oxford R&D Cold Fibre radiation tests Splitter and connector radiation tests Fibre reliability after radiation.
Slide 1 5th LHC RADIATION WORKSHOP, CERN, , Jochen Kuhnhenn, Fraunhofer INT Radiation tolerant fibres for LHC controls and communications.
Tecnologica Componentes Electrónicos, S.A. Workshop - Laser diodes in Space Slide No: 1 Date: May 11 – 12, 2006 Componentes Electrónicos, S.A. Juan Barbero.
UNIT-II Optical Fiber ECE – IV SEM Manav Rachna College of Engg.
STATUS ON Optical fiber: Preliminary tests on Optical Fiber and Fiber Optic Feedthrough Massimo Rossella, Marco Prata, Tommaso Cervi INFN, Sezione di Pavia.
1 Optical fiber irradiation tests 1.Results from ATLAS LAr 2.Narrow down to Germanium doped GRIN fiber 3.Preliminary tests 4.Tests in the plan Jingbo Ye.
Update on Optical Fibre issues Rainer Schwemmer. Key figures Minimum required bandwidth: 32 Tbit/s –# of 100 Gigabit/s links > 320, # of 40 Gigabit/s.
Radiation Tests on optical fibres for the LHC machine T. Wijnands, D. Ricci CERN EN department Fraunhofer INT.
WACH4 26/11/2002Julien Cogan CERN/EP/CMA-1- THERMAL STEPS ANALYSIS Goals & Means : –apply a “step function” on the cooling water –look at : APD response.
Optical Communications for Future Trackers ANL/FNAL/UC/VWS Meeting Nov., 2011 Alan Prosser CD/ESE Fermilab 1.
Radiation Test Results Preliminary measurements from exposure to gamma rays at SCK-CEN B. Todd Huffman, C. Issever, T. Weidberg Summer Students - A. Povey,
1 Roger Rusack The University of Minnesota. Projects  Past Projects  11,000 channels of 0.8 Gbs for the CMS crystal calorimeter readout.  1,500 channels.
Application of photodiodes
Distributed Optical Fibre Radiation and Temperature Sensor (DOFRS)
Practical advices for using TCT (mostly for Particulars setups)
Current Situation of Yb:YAG Laser at A1 Ground Laser Hut
Using diode laser for atomic physics (I)
Next generation rad-hard links
Fiber optic sensors integration in magnets and in test facilities
2 Fraunhofer INT Euskirchen Germany
CERN Conductor and Cable Development for the 11T Dipole
Optical Amplifier.
INVERSE BUILDING MODELING
PIN DIODE.
Sandis Spolitis, Inna Kurbatska, Vjaceslavs Bobrovs
The Optical Fiber and Light Wave Propagation
Presentation Title Goes Here
Sensitivity of quantum dot semiconductor lasers to optical feedback
A. Bramati M. Romanelli E. Giacobino
Design of Optical Digital Transmission Systems
RF cables calibration Matteo Volpi Thomas Geoffry Lucas
Making Networks Light March 29, 2018 Charleston, South Carolina.
W. Ali, R. Corsini, E. Ciaramella SSSA Pisa Italy
Characterizing FOX Demonstrator Test Setups for LArDPS to FEX Modules at CERN RuthAnn Gregory.
CW accelerating module test progress at DESY
High Power, Uncooled InGaAs Photodiodes with High Quantum Efficiency for 1.2 to 2.2 Micron Wavelength Coherent Lidars Shubhashish Datta and Abhay Joshi.
Radiation tolerant fibres for LHC controls and communications
Introduction to Fiber Optics
Design of Optical Digital Transmission Systems
ENGINEERING PHYSICS B.TECH :I YEAR SEM-I MECHANICAL & CIVIL
Fiber Optic Transmission
Program of Studies − microscopes and telescopes
Optical fiber based sensors for low temperature and superconductors
K. Gill, G. Cervelli, R. Grabit, F. Jensen, and F. Vasey. CERN, Geneva
Geoscience Text Images & Small Group Discussion
Presentation transcript:

SLHC Radiation Test Results Preliminary measurements Versatile Link project from exposure to gamma rays at SCK-CEN B. Todd Huffman (speaker), J. Hanzlik, C. Issever, T. Weidberg 24/09/09 B. Todd Huffman

The Outline Brief explanation of facility used SCK-CEN sources Test procedures then and now. Some Previous results and motivation for temperature controlled tests Tests of Mulit-mode fibres Draka RHP-1 SRH InfinicorSX+ Conclusions 24/09/09 B. Todd Huffman

The two locations: 60Co g rays RITA 0.6kGy/hr BRIGITTE 20kGy/hr 24/09/09 B. Todd Huffman

Previous High-dose test result Draka Commercial Draka 3 Infinicor Draka RHP-1 SRH 24/09/09 B. Todd Huffman

These Results are Good Good Candidate MM fibres identified InfinicorSX+ and Draka RHP-1 Draka Fibre is under further development and will require future tests But Limitations of Previous tests have prompted further studies. Temperature dependence in particular 24/09/09 B. Todd Huffman

RIA and temperature, 1st 6 hours. 24/09/09 B. Todd Huffman 7

Previous research on RIA in fibre Single-mode Multi-mode 850 nm GRIN fibre at room temp (curve C) and -17 C (curves A & B) credit: Thériault Radiation effects on COTS laser-optimized graded-index multimode fibers exposed to intense gamma radiation fields Single-mode RIA as fcn of temp. credit: Kanamori et al. Transmission Characteristics and Reliability of Pure Silica-Core Single-Mode Fibers RIA is temperature-dependent! 24/09/09 B. Todd Huffman 8

Cold Container designed Uses Peltier cooling elements 4 coolers – 15V and 7A operation Direct connection to Draka fibre DT = ~60 deg C Able to remove ~40W heat load Suitable only for low dose facility Radiation Damage and heat load Heat shed to the shielding water Water ambient temp = 30 deg C. Goal  Maintain -250C 24/09/09 B. Todd Huffman

Container to Actively Cool Fibres 24/09/09 B. Todd Huffman

InfinicorSX+ Temperature Effects 24/09/09 B. Todd Huffman

Draka Fibre Temperature Effects 24/09/09 B. Todd Huffman

An interesting Temp. Radiation effect Prior to radiation, fibre attenuation relatively insensitive to temperature variations. RIA sensitizes fibres to temperature. Particularly Dramatic with Infinicor fibres Present, but less of an effect with Draka fibres Keep in mind 50m of fibre are used. 24/09/09 B. Todd Huffman

Before 0.01 dB 0.05 Deg. C 24/09/09 B. Todd Huffman

after 0.7 dB 0.05 Deg. C 24/09/09 B. Todd Huffman

0.05 dB Before 1 Deg. C 24/09/09 B. Todd Huffman

after 0.2 dB 1 Deg. C 24/09/09 B. Todd Huffman

Comparisons, InfinicorSX+ T = +300 C Dose = 65 kGy(Si) Gamma source at room temperature. Variation is from prev. Stability limitations. T = -23.30 C Dose = 30 kGy(Si) 24/09/09 B. Todd Huffman

Comparisons, InfinicorSX+ T = +300 C Dose = 65 kGy(Si) Gamma source at room temperature. Variation is from prev. Stability limitations. T = -23.30 C Dose = 30 kGy(Si) 24/09/09 B. Todd Huffman

Draka RHP-1 SRH fibre T = -40 C Total Dose ~ 15 kGy(Si) T = -250 C 24/09/09 B. Todd Huffman

Attenuation Upper limits Low doses  extrapolate linearly up to SLHC tracker doses 375kGy. CAUTION!!: upper limit Lower dose rate in Tracker volume RIA follows logarithmic scale at high dose At -250C inside Tracker volume InfinicorSX+  1.1 dB Warm result  0.24 dB Draka RHP-1  0.6 dB 24/09/09 B. Todd Huffman

Conclusions Infinicor Fibre is Ge doped Draka Fibre is F doped No Ge used Neither uses Phosphorous in their manufacturing process F doped fibre (Draka) has better radiation performance even at cold temperatures ~0.05 dB/m vs. ~0.08 dB/m after 30kGy integrated exposure. 24/09/09 B. Todd Huffman

Conclusions Are we Qualified for operation of these fibres at Cold Temperatures? Definite Maybe. Extrapolation very conservative, but very dodgy Ideally we would obtain close to a full SLHC dose (~400kGy) cold Brigitte can do this Smaller volume. Potentially higher heat load. Peltier system would surely fail. 24/09/09 B. Todd Huffman

Conclusions We believe a CO2 thermal management system can achieve the same goal at the higher dose facility. Studying the feasibility of this. Back-up is to use dry-ice. Previous tests show we obtain -780C for 24 hours even with heat load. But, such a test would teach us little if fibre ends up with more than 1dB/m RIA. 24/09/09 B. Todd Huffman

General future Cold tests finished by April Qualified two fibres Re-qualify Draka fibre with higher bandwidth Move to qualifications of PLC splitters, LC connectors, full cabling solutions Mechanical tests 24/09/09 B. Todd Huffman

Next Slides are backup slides End Of Talk Next Slides are backup slides 24/09/09 B. Todd Huffman

Optical Patch cables Splitter No Longer used! Conn. 24/09/09 B. Todd Huffman

System Stability tests – last year Ran system for extended time periods. Found stability limitations Extensive tests by J. Hanzlik showed the optical splitter was the main cause of instability. ±1.5 dB absolute stability limitation for MM fibres. 24/09/09 B. Todd Huffman

Stability of test system Output from multi-mode fibre (coupler in system) VCSEL coupler PD PD = photo-diode 1.5 dB 0.2 = connector Output from multi-mode fibre (no coupler in system) -.11 VCSEL PD dB -.15 PD = photo-diode = connector Removing coupler seems to improve stability of MM system 24/09/09 B. Todd Huffman 12

Stability by the Numbers Multi-mode fibre InfinicorSX+ RMS variation using 1x4 optical splitter ~0.15 dB RMS variation of single channel – no splitter ~0.0053 dB Single Mode fibre SMF-28 RMS variation using 1x4 optical splitter ~0.014 dB RMS variation of Single channel ~0.042 dB 24/09/09 B. Todd Huffman

You can even watch it turn on. RIA oscillations increase in amplitude Temp. oscillates & rad. starts 24/09/09 B. Todd Huffman

Semi-cold Draka Run -4 deg C 24/09/09 B. Todd Huffman

Behavior of Reference fibres Attenuation, dB Attenuation, dB 24/09/09 B. Todd Huffman

InfinicorSX+ Temperature Effects 24/09/09 B. Todd Huffman

Draka RHP-1 SRH fibre T = -40 C T = -250 C 24/09/09 B. Todd Huffman