CTA-LST Large Size Telescope M. Teshima for the CTA Consortium Institute for Cosmic Ray Research, University of Tokyo Max-Planck-Institute for Physics.

Slides:



Advertisements
Similar presentations
Enrico Giro – INAF – OAPD - ASTRI general meeting #9– Bologna, 24 Feb Towards the upgrade of the ASTRI structure following the consolidation of.
Advertisements

CMSC 2006 Orlando Active Alignment System for the LSST William J. Gressler LSST Project National Optical Astronomy Observatory (NOAO) Scott Sandwith New.
All-aluminum mirrors for the MAGIC Cherenkov Telescope
FDWAVE : USING THE FD TELESCOPES TO DETECT THE MICRO WAVE RADIATION PRODUCED BY ATMOSPHERIC SHOWERS Simulation C. Di Giulio, for FDWAVE Chicago, October.
Calibration for LHAASO_WFCTA Yong Zhang, LL Ma on behalf of the LHAASO collaboration 32 nd International Cosmic Ray Conference, Beijing 2011.
Optical Astronomy Imaging Chain: Telescopes & CCDs.
Cut off more slowly ~ 50GeV Thompson astro-ph/ Credit: A.K. Harding (NASA/GSFC) Our first target: Crab pulsar/nebula The standard candle for gamma-ray.
Mathieu de Naurois, H.E.S.S.High Energy Phenomena in the Galacic Center H.E.S.S. Observations of the Galactic Center  The H.E.S.S. Instrument.
Transient Science with the Allen Telescope Array Geoff Bower Berkeley.
Large Magellanic Cloud, 1987 (51.4 kparsec) SN 1987a after before 2006 Hubble.
H.E.S.S. High Energy Stereoscopic System Jon Cerny Bancroft-Rosalie School August 2002.
The Highest Energy Cosmic Rays Two Large Air Shower Detectors
Panorama of the Universe: Daily all-sky surveys with the SKA John D. Bunton, CSIRO TIP, Ronald D. Ekers, CSIRO ATNF and Elaine M. Sadler, University of.
This Set of Slides This set of slides deals with telescopes. Units covered: 26, 27, 28, 29, and 30.
On A Large Array Of Midsized Telescopes Stephen Fegan Vladimir Vassiliev UCLA.
X-ray Timing and Polarization mission & instrumentation DONG Yongwei Center for Particle Astrophysics Institute of High Energy Physics, Chinese Academy.
F. Goebel, MPI München, 4 May 2006, Berlin Florian Goebel Max-Planck-Institut für Physik (Werner-Heisenberg-Institut) München for the MAGIC collaboration.
22 February 2006 Quo Vadis ? Wide Field Imaging A Wide Angle Very Low Threshold Air Cherenkov Imaging Telescope Razmick Mirzoyan MPI Munich, Germany.
17 November 2003EUSO meeting: R. Mirzoyan The MAGIC Telescope Project Razmick Mirzoyan Max-Planck-Institute for Physics Munich, Germany EUSO meeting.
Optics for Wide Field X-ray Imaging
Wilga 2007 π of the Sky Full π system and simulation Janusz Użycki Faculty of Physics Warsaw University of Technology.
May 4-5, 2006 T.Schweizer, CTA meeting Berlin Concept idea for a future telescope array observatory CTA meeting Berlin May 4-5, 2006 Thomas Schweizer.
Observations of 3C 279 with the MAGIC telescope M.Teshima 1, E.Prandini 2, M.Errando, D. Kranich 4, P.Majumdar 1, M.Mariotti 2 and V.Scalzotto 2 for the.
Gus Sinnis RICAP, Rome June 2007 High Altitude Water Cherenkov Telescope  Gus Sinnis Los Alamos National Laboratory for the HAWC Collaboration.
SPIE Optics for EUV, X-Ray, and Gamma-Ray Astronomy VI
Improved PMTs for the Cherenkov Telescope Array project Razmik Mirzoyan for the Focal Plane Instrumentation WG Max-Planck-Institute for Physics Munich,
Performance of CRTNT for Sub-EeV Cosmoc Ray Measurement Zhen Cao IHEP, Beijing & Univ. of Utah, SLC Aspen, CO, 04/2005.
EAS Reconstruction with Cerenkov Photons Shower Simulation Reconstruction Algorithm Toy MC Study Two Detector Configuration Summary M.Z. Wang and C.C.
Argonne / U. Chicago Initiative on R & D for Next Generation Ground Based Gamma-ray Particle Astrophysics/Astronomy Karen Byrum Jun 7, 2010 Argonne National.
May 4th 2006R.Mirzoyan: CTA meeting, Berlin The MAGIC Project: Performance of the 1st telescope Razmick Mirzoyan On behalf of the MAGIC Collaboration Max-Planck-Institute.
CTA The next generation ultimate gamma ray observatory M. Teshima Max-Planck-Institute for Physics.
M.Teshima MPI für Physik, München (Werner-Heisenberg-Institut) for MAGIC collaboration MAGIC.
Gus Sinnis Asilomar Meeting 11/16/2003 The Next Generation All-Sky VHE Gamma-Ray Telescope.
Ultra High Energy Cosmic Rays -- Origin and Propagation of UHECRs -- M.Teshima Max-Planck-Institut f ü r Physik, M ü nchen Erice Summer School July
LOFAR LOw Frequency Array => most distant, high redshift Universe !? Consortium of international partners… Dutch ASTRON USA Haystack Observatory (MIT)
Silicon Optics for Wide Field X-ray Imaging Dick Willingale et al. – SPIE August 2013 Silicon Optics for Wide Field X-ray Imaging Dick Willingale University.
The MAGIC Telescope MAGIC
1 Status of the CANGAROO-III Project Masaki Mori ICRR, University of Tokyo International Symposium on High Energy Gamma-Ray Astronomy, June 26-30, Heidelberg.
Extending the Sensitivity Of Air-Cerenkov Telescopes Steve Biller, Oxford University (de la Calle & Biller – astro-ph/ )
AROMA-W Ichiro Takahashi Takanori Sakamoto for the AROMA team (Aoyama Gakuin University)
HAWC Science  Survey of 2  sr (half the sky) up to 100 TeV energies Probe knee in cosmic ray spectrum Identify sources of Galactic cosmic rays  Extended.
Use LL1 & LL6 to detect microwave radiation equipping the empty pixels with microwave radio receivers Pixels without photomultipliers (removed to be installed.
1 João Espadanal, Patricia Gonçalves, Mário Pimenta Santiago de Compostela 3 rd IDPASC school Auger LIP Group 3D simulation Of Extensive Air.
Introduction Data analyzed Analysis method Preliminary results
Polarization Characteristic of Multi-layer Mirror for Hard X-ray Observation of Astrophysical Objects T. Mizuno 1, J. Katsuta 2, H. Yoshida 1, H. Takahashi.
EUSO Atmospheric Monitoring from Space M.Teshima on behalf of the EUSO collaboration MPI für Physik, München (Werner-Heisenberg-Institut)
FSC Status and Plans Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group PANDA Russia workshop, ITEP 27 April 2010.
June 6, 2006 CALOR 2006 E. Hays University of Chicago / Argonne National Lab VERITAS Imaging Calorimetry at Very High Energies.
Goals for HETDEX Determine equation of state of Universe and evolutionary history for dark energy from 0
05/02/031 Next Generation Ground- based  -ray Telescopes Frank Krennrich April,
Contratto ASI/Luna Astrofisica delle Alte Energie.
Performance of GeV gamma ray camera for SUBARU optical-infrared telescope A.Asahara*, K.Komiyama#, G.Kosugi#, H.Kubo*, S.Miyazaki#, M.Mori , M.Nakagiri#,
Status of the MAGIC Telescope Project Presented by Razmick Mirzoyan On behalf of the MAGIC Collaboration Max-Planck-Institute for Physics (Werner-Heisenberg-Institute)
Exploring an evidence of supermassive black hole binaries in AGN with MAXI Naoki Isobe (RIKEN, ) and the MAXI
MAGIC Telescopes - Status and Results 2009/ Isabel Braun Institute for Particle Physics, ETH Zürich for the MAGIC collaboration CHIPP Plenary Meeting.
The CRTNT Project (Cosmic Ray & Tau Neutrino Telescope) --- sensitivity and prototype experiment Huihai He, IHEP, CAS On behalf of the CRTNT collaboration.
Report by LST-SYS coordinator M.Teshima Max-Planck-Institute for Physics.
Astronomical Spectroscopic Techniques. Contents 1.Optics (1): Stops, Pupils, Field Optics and Cameras 2.Basic Electromagnetics –Math –Maxwell's equations.
Candidate light sensors for CTA High precision measurements of ultra-low light level detectors for CTA project: PMTs and SiPMs Matthias Kurz Max-Planck-Institute.
A SUPER-WIDE FIELD OF VIEW CHERENKOV TELESCOPE J. Cortina, R. López-Coto, A. Moralejo. R. Rodríguez Pizza seminar June 3 rd, 2015.
H.Ohoka, H.Kubo, M.Aono, Y.Awane, A.Bamba, R.Enomoto, D.Fink, S.Gunji, R.Hagiwara, M.Hayashida, M.Ikeno, S.Kabuki, H.Katagiri, K.Kodani, Y.Konno, S.Koyama,
Future Imaging Atmospheric Cherenkov Telescopes:
B. Humensky 2/24/2012 CTA-SCT Mtg - SLAC
L.L.Ma for LHAASO collaboration Beijing China
Expectation of Cosmic Ray Energy Spectrum with LHAASO
MAGIC M.Teshima MPI für Physik, München (Werner-Heisenberg-Institut)
performance requirements technical specifications
Cherenkov Telescope Array
HAWC Science Survey of 2p sr up to 100 TeV energies Extended Sources
(National Astronomical Observatory of Japan)
Presentation transcript:

CTA-LST Large Size Telescope M. Teshima for the CTA Consortium Institute for Cosmic Ray Research, University of Tokyo Max-Planck-Institute for Physics

Large Size Telescope (LST) in CTA MST 10-12m LST 23m SST 4-6m North: Canaries / Mexico South: Namibia / Chile / Argentina LST 23m MST 10-12m SST 4-6m Two stations for all sky observatory

Science case of LST LST is optimized in the energy range between GeV LST is optimized in the energy range between GeV Low energy threshold Low energy threshold Trigger threshold: GeV Trigger threshold: GeV Analysis threshold: GeV Analysis threshold: GeV key physics cases: key physics cases: High-redshift AGNs and GRBs High-redshift AGNs and GRBs Binaries, Pulsars and other type of transients at low energy Binaries, Pulsars and other type of transients at low energy High redshift AGNs (z<3) GRBs (z<10) Pulsars Binaries and transients

Specifications/Requirements of LST Diameter: 23m Diameter: 23m Dish area: 400 m 2 Dish area: 400 m 2 F/D = 1.2, F=28m F/D = 1.2, F=28m Dish profile: Parabolic Dish profile: Parabolic FOV = 4.5 degrees, Pixel size = 0.1 degrees (~2500ch camera) FOV = 4.5 degrees, Pixel size = 0.1 degrees (~2500ch camera) Fast rotation: <180 deg/20 sec Fast rotation: <180 deg/20 sec Dish profile: parabolic  isochronicity: <0.6 ns RMS Dish profile: parabolic  isochronicity: <0.6 ns RMS Camera sagging: < 1-2 pixels Camera sagging: < 1-2 pixels Camera oscillation in wind gust: <8mm Camera oscillation in wind gust: <8mm  Active oscillation damping by LAPP IN2P3 Designed by MPI Munich

LST 23m size mirror reflector 198 Hex-shape segmented mirrors of 1.5m size 198 Hex-shape segmented mirrors of 1.5m size Total area 〜 400m 2 Total area 〜 400m 2 Central hole for the calibration Central hole for the calibration Permanent AMC (Active Mirror Control) Permanent AMC (Active Mirror Control) 1.5 m Hex Mirror prototype by CTA-Japan Wavelength (nm) Reflectivity (%) SiO2, HfO2 multi-coating

Optical axis and permanent AMC Define optical axis with the IR Laser beams Define optical axis with the IR Laser beams High precision inclinometer (a few arcsec)  zenith angle High precision inclinometer (a few arcsec)  zenith angle HR CCD camera at the center of dish to monitor the optical axis and star field  pointing direction in sky HR CCD camera at the center of dish to monitor the optical axis and star field  pointing direction in sky (Camera LED position) – (Optical axis Laser position)  camera sag (Camera LED position) – (Optical axis Laser position)  camera sag (Mirror Laser positions) – (Optical axis Laser position)  misalignments of mirror directions (Mirror Laser positions) – (Optical axis Laser position)  misalignments of mirror directions Target LED OA-Lazer MIR-Lazers SKY MIR-Lazers Stars IMAGE with HR CCD Camera PMT - CAMERA

Demonstration of Active Oscillation Damping System for the LST Arch by LAPP IN2P3

Gamma/Hadron Separation below 100GeV Scaled width (below 50GeV) 50GeV gamma ray images with LSTs Height of Shower Maximum gamma Hadron

Optimization of Telescope geometry Ø 1° source

Camera, clusters and Cooling Sealed Camera (MAGIC-II camera) Size: 2.5 m Weight: 2 tons # of Ch: ~ 2500 ch Heat: ~ 5000W Cluster Prototype by CTA-Japan (R.Orito: #1091) 7PMTs CW HV system Pre-Amplifier DRS-4 readout system (4μsec) G-bit ethernet Water cooling System

Differential Sensitivity of 4 x LSTs Below 200GeV LSTs will have a good sensitivity Configuration E LST x 4, MST x 23, SST 32

CTA Monte Carlo: Expected Light curve for GRB at z=4.3 CTA performance study by S.Inoue, Y.Inoue, T.Yamamoto, et al

Summary CTA-LST will provide a fairly good sensitivity between 20GeV and 200GeV CTA-LST will provide a fairly good sensitivity between 20GeV and 200GeV CTA Science will be expanded to the new domain CTA Science will be expanded to the new domain High redshift AGNs (z<3), GRBs(z<10), Pulsars, Galactic Transients High redshift AGNs (z<3), GRBs(z<10), Pulsars, Galactic Transients CTA-LST baseline design CTA-LST baseline design Diameter 23m, Focal length 28m, F/D = 1.2 Diameter 23m, Focal length 28m, F/D = 1.2 FOV 4.5 degrees, Pixel size 0.1 degrees FOV 4.5 degrees, Pixel size 0.1 degrees Many new proven technologies will be implemented Many new proven technologies will be implemented Space frame structure with CFRP Space frame structure with CFRP Total weight ~ 50 tons  180 degrees/20sec Total weight ~ 50 tons  180 degrees/20sec Permanent active mirror control Permanent active mirror control Permanent camera oscillation damping system Permanent camera oscillation damping system Sealed camera with water cooling system Sealed camera with water cooling system 1GHz sampling DRS4 system with 4μsec deep memory 1GHz sampling DRS4 system with 4μsec deep memory

Optical axis and permanent AMC Define optical axis with the IR Laser beams Define optical axis with the IR Laser beams High precision inclinometer (a few arcsec)  zenith angle High precision inclinometer (a few arcsec)  zenith angle HR CCD camera at the center of dish to monitor the optical axis and star field  pointing direction in sky HR CCD camera at the center of dish to monitor the optical axis and star field  pointing direction in sky (Camera LED position) – (Optical axis Laser position)  camera sag (Camera LED position) – (Optical axis Laser position)  camera sag (Mirror Laser positions) – (Optical axis Laser position)  misalignments of mirror directions (Mirror Laser positions) – (Optical axis Laser position)  misalignments of mirror directions