Atmospheric Super Test Beam for the Pierre Auger Observatory

Similar documents
Customized LIDARs. Research Pollution Climate. Raman, Depolarization, Backscatter, DIAL

Customized LIDARs. Research Pollution Climate. Raman, Depolarization, Backscatter, DIAL

ARCADE status. L. Valore. University of Naples - INFN Naples

TacBio: A UV-based Biological Aerosol Detector. TacBio Overview Page 1

Product data sheet Palas Fidas 200 S

Multitel develops components and full instruments for in-vitro and in-vivo diagnostics in the biomedical, food and drug sectors.

POWER & ENERGY METERS BEAM PROFILING THZ MEASUREMENT COMPANY PROFILE

New remote sensing instruments for water vapour monitoring developed at EPFL

Laser Diagnostics and Optical Measurement Techniques

Range Dependent Turbulence Characterization by Co-operating Coherent Doppler Lidar with Direct Detection Lidar

POWER & ENERGY METERS BEAM PROFILING THZ MEASUREMENT COMPANY PROFILE

The FEL Facility Optical Diagnostics and FEL Characterization

CART and GSFC Raman Lidar Measurements of Atmospheric Aerosol Backscattering and Extinction Profiles for EOS Validation and ARM Radiation Studies

Analisi del Focus-shift su sorgenti multikw. Luca Porcelluzzi Ophir Spiricon Europe GmbH

state of the art methane leak detection CHARM and GasCam 2011 October 13 th Dr. Axel Scherello

Our photo detectors are offered for both power or energy measurements. Measure as low as a few femtojoules in energy or a few picowatts in power.

SOLUTION MINING RESEARCH INSTITUTE

Laser Safety and Classification Full Version (CA-1110) Advanced Version (CA-1111) Basic Version (CA-1112)

WHAT IS LASER ULTRASONIC TESTING?

POWER & ENERGY METERS BEAM PROFILING THZ MEASUREMENT COMPANY PROFILE

Our photo detectors are offered for both power or energy measurements. Measure as low as a few femtojoules in energy or a few picowatts in power.

EARLINET products for model evaluation and assimilation

DWDM OTDR with Tunable Laser MTP-200-D100. Hand-held High Performance OTDR. Series

Remote Detection of Leaks in Gas Pipelines with an Airborne Raman Lidar. Strategic Insights, Volume VII, Issue 1 (February 2008)

The Optical Scattering Calibration System at SNO+ IOP 2015

Product data sheet Palas Promo 2000

Development of On-line Instrumentation and Techniques to Detect and Measure Particulates

Praetorian Fibre Optic Sensing

FLIM/FFS and Nanoimaging Upgrade of Olympus confocal microscopes

Recent Advances in Solid State Lasers and Nonlinear Optics for Remote Sensing

Measurement of light scattering in deep sea

COMPACTNESS 34.1 PERFORMANCE ANTICIPATION

Customized MCPs for Analytical Instruments. An MCP for every application

Developments Towards a Spacebased Wind Lidar for the International Space Station

TSI AEROTRAK PORTABLE PARTICLE COUNTER MODEL 9110

COMPACTNESS 34.1 PERFORMANCE ANTICIPATION

The new generation Teledyne NIR detectors for the SNAP/JDEM mission spectrograph.

Compact Sensor Heads for In-situ and Non-Contact Standoff Gas Sensing using TDLAS in Harsh Environments

Spectrum Detector, Inc.

Chemistry Instrumental Analysis Lecture 4. Chem 4631

Industrial presentation. Philippe Marchais - July 3rd, NDIP Tours

LCLS Instruments. Jerry Hastings June 20, 2008 LCLS

E11 Tests of trace gas concentration multicomponent. monitoring system

State of the Corona Camera Industry Past, Present and Future RIAAN ROSSOUW

Low-Frequency Raman Spectroscopy Enabling Affordable Access to the Terahertz Regime

Link loss measurement uncertainties: OTDR vs. light source power meter By EXFO s Systems Engineering and Research Team

OptoYag M. clear vision

WHITE PAPER FIBER OPTIC SENSING. Summary. Index. Introduction. About Fischer Connectors

Laser Damage Measurements

Passive Standoff FTIR Detectors as Transducers. Background From radiation to information

RAMAN SPECTROSCOPY See more, faster than ever before

Variable Temperature Options for Optical Experiments

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

Smart Fire Prevention

Laser Radiation and High Voltage/Electrical Shock. Disclaimer and Limitation of Liability. Shipping Damage. Trademarks

Omnisens DITEST TM FIBER OPTIC DISTRIBUTED TEMPERATURE & STRAIN SENSING TECHNIQUE

Lasers Technical Seminar at Bruno Events Center on March 27 th, Next generation of SPADs - Single Photon Avalanche Detectors

An overview of the Science and Technology Facilities Council capabilities in healthcare

CCD and CID solid-state detectors

Ultraviolet radiation detector to obtain the rate of particles at different heights

Optical Techniques for Industrial Inspection

The LHCb Outer Tracker: Production & Ageing studies

Today s Outline - September 12, C. Segre (IIT) PHYS Fall 2016 September 12, / 21

Customization of Optoelectronic Detectors Part Two in a Six-Part Series

Stand-off Detection of Trace Explosives by Infrared Photothermal Imaging. Trace Contamination

Correlation-based OTDR for in-service monitoring of 64-split TDM PON

The New DUSTTRAK II and DRX Aerosol Monitors

mach 5 100kHz Digital Joulemeter: M5-SJ, M5-IJ and M5-PJ Joulemeter Probes

Building and Characterizing 14GHz InGaAs Fiber Coupled Photodiodes

The FireBird mission - a scientific mission for Earth observation and hot spot detection

Fiber optic distributed pressure sensor for structural monitoring applications

The distributed particle detectors and data acquisition modules for Extensive Air Shower measurements at "HT-KZ" experiment

The New DUSTTRAK II and DRX Aerosol Monitors

iotdr Series Portable OTDR Test Set iotdr Series OTDR Tester is entirely new portable product released by OPWILL.

Experimental Study to Evaluate Smoke Stratification and Layer Height in Highly Ventilated Compartments

Beam Analysis nm and µm - Pyroelectric Array Camera. Pyrocam TM IIIHR & Pyrocam IV Series

Laser Particle Size Analyzer

High-Power Q-Switched Diode-Pumped UV Laser Q-Series, Q305

HDCVI PIR Camera User s Manual

LM-80V , h V LM-30V h V

FTB-730 PON FTTx/MDU OTDR OPTIMIZED FOR ACCESS FIBER DEPLOYMENTS AND TROUBLESHOOTING

Current Research Topics in Optical Sensors and Laser Diagnostics

Application Note. Which characterization method is best for your application? The Future of Thermal Imaging is Here!!!

LHCb Rich Detectors Control and High Voltage Systems

Understanding total measurement uncertainty in power meters and detectors

FEE Diagnostics and Commissioning. June 17, 2008

clear & preserve vision OptoYag&SLT

Status of the PRad Experiment (E )

AEROSOL SPECTROMETERS

818E Series Energy Detector. User s Manual

Beam Analysis nm and µm - Pyroelectric Array Camera. Pyrocam TM IIIHR & Pyrocam IV Series

MX1A and MX1B: Laser Displacement Detection Sensors. 85% to 110% of the rated voltage MX1A: 15VA, MX1B: 25VA

LAB REPORT SUBMISSION COVER PAGE ETN4106 OPTOELECTRONICS AND OPTICAL COMMUNICATIONS

Development of high sensitivity radon detectors

Clearlite Photonic Fibers

818 Series. Low-Power Detectors ABSOLUTE SPECTRAL RESPONSIVITY (A/W)

Instruments Designed for POF & Fibre Optic Cable Testing

Compact Raman spectrometer system for low frequency spectroscopy

Ocean Visuals early warning of oil spills and environmental monitoring

64 Max IR Thermometer

Transcription:

Atmospheric Super Test Beam for the Pierre Auger Observatory L. Wiencke for the Pierre Auger Collaboration and A. Botts, C. Allan, M. Calhoun, B. Carande, M. Coco, J. Claus, L. Emmert, S. Esquibel, L. Hamilton, T.J. Heid, F. Honecker, M. Iarlori, S. Morgan, S. Robinson, D. Starbuck, J. Sherman, M. Wakin, O. Wolf Lawrence Wiencke Colorado School of Mines ICRC2011, Beijing 1

UV Pulsed Laser test beams 50 EeV EAS 16 km Vertical 5 mj Laser 27 km (50 shot average) 50 EeV EAS 28 km Some applications atmospheric monitoring 1 timing, geometry, aperture Comparison of laser and air shower light profiles 5 mj Laser ~ 100 EeV Air Shower (scattering) (fluorescence) 1 K. Loudec for the Pierre Auger Collaboration, poster 568. 2

Atmospheric Super Test Beam Solid State UV Laser + Robotic Calibration + Raman LIDAR receiver 355 nm Stable No moving parts Passive cooling 1-100 Hz Energy Polarization at ground (z=0) τ(z) aerosol optical depth Best practices method Independent water vapor (z) 3

Atmospheric Super Test Beam Solid State UV Laser + Robotic Calibration + Raman LIDAR receiver 355 nm Stable No moving parts Passive cooling 1-100 Hz Energy Polarization at ground (z=0) τ(z) aerosol optical depth Best practices method Independent water vapor (z) Nγ(z) Nγ(z=0) τ(z) 4

Why Raman LIDAR? Elastic Raman 20 μm 5 μm 2 Unknowns Electron Scanning Images 1 Unknown Transmission of Aerosol Particles from Transmission Pierre Auger Observatory Scattering (M. Micheletti) 5

Components tested in the Pierre Auger R&D site in Southeast Colorado USA Also see F. Sarazin for the Pierre Auger Collaboration New technologies for the Pierre Auger Observatory Research and development in southeastern Colorado (RDA) Poster 922. 6

DLF N For this test compare measurements of Aerosol Optical Depth τ(z) by two independent detectors T=e -τ(z)/sinѳ AMT Ѳ 7

Extracting Aerosol Optical Depth τ(z) T=e -τ(z)/sinѳ LIDAR (Raman Back Scatter) LIDAR and retrieval algorithm have been benchmarked against EARLINET EARLINET: European Aerosol Research LIDAR Network to Establish an Aerosol Climatology AMT (Elastic Side Scatter) Method used with Auger Observatory Fluorescence Detector + Central Laser Data Normalized Method L. Valore for the Pierre Auger Collaboration, Proc. 31 st ICRC, Łódź, Poland, 2009 (arxiv:0906.2358[astroph]) Astropart. Phys, 2010 33, 108-129 2009 (arxiv:1105.4016 [astro-ph]). 8

AMT: Atmospheric Monitoring Telescope WiFi 3.5 m 2 mirror (HiRes Optics) 1x1 degree Pixels GPS Based Trigger HEAT Electronics [1] 20 Mhz [1] H.J. Mathes presentation 0761 9

Laser/LIDAR (39 km Distant) 10

Raman LIDAR/Laser Liquid Light Guide UV window Automated Hatch GPS Slow Control Receiver Solid State Laser (355 nm, 7 ns) 5 mj 100 Hz/ 4 Hz Energy Monitor Mirror 50 cm, f/3 Data Acquisition Fast Photon Counting 250 Mhz 11

3-Channel LIDAR Receiver 355 nm Elastic Scattering 407.5 nm Raman H 2 0 Scattering Light Guide 386.7 nm Raman N 2 Scattering 12

Average difference in air density as determined from the GDAS model and measured from 27 radiosonde launches. +/- 0.25 % Details: M. Will for the Pierre Auger Collaboration, Poster 0339 13

Data Accumulation Hours with AMT and LIDAR observing 14

τ(4.5 km) 15

τ(z=4.5 km) Raman LIDAR τ(z=4.5 km) AMT 16

Atmospheric Super Test Beam - Status Raman LIDAR Weather Station Insulation Laser, Calibration Thermal Reservoir Batteries Nev DeWitt Pierrat, Blake Knoll (CSM) Funded, Construction in progress, Ship to Argentina, Install at CLF site 2012 17

Summary/Conclusions Accumulated >200 hours of data with AMT and Raman LIDAR First comparison between Raman and Elastic Side Scattering techniques Correlation observed Super Beam System Independent measurement of τ(z,t), especially after interesting events Test beam with Nγ known at ground and vs height Funded, construction in progress Inter disciplinary Science relatively few aerosol profile instruments in the southern hemisphere. 18

Extra Slides 19

Calibration and Monitoring Network Camera Cloud Monitor High Voltage Monitor AMT Laser/ LIDAR 20

21

Physics Analysis with Auger Fluorescence Detector Typically select periods with τ(4 km) < 0.1 τ(4.5 km) 22

23

large particles LR 10 30sr desert aerosols LR 35 45sr continental aerosols LR 50 70sr dust or polluted aerosol LR 80 100sr τ(4.5 km) 24

Operations Minute 0 15 30 45 60 AMT +Laser 120 Shots AMT LED Calib. Vary Raman LIDAR Laser @ 100 Hz Hours with AMT and LIDAR observing 25

26 Atmospheric Soundings Profiles: Temperature Pressure Water vapor Wind Density Depth