October 20-21, 2005 “Towards the Future” Workshop Andrew Smith mini- High Altitude Water Cherenkov experiment e   145 meters 4 meters  Andrew Smith.

Slides:



Advertisements
Similar presentations
Latest results from ARGO-YBJ P. Camarri University of Roma “Tor Vergata” And INFN Roma Tor Vergata P. Camarri - WAPP Darjeeling, India - Dec 17-19,
Advertisements

Los Alamos National Laboratory Adelaide, Australia. December 2006 Gus Sinnis Synoptic TeV Telescopes Results from Milagro Plans for HAWC.
WP-Technology Working Group Future of Ground Based Gamma-ray Astronomy Feb 8, Technology & Cost WP Working Group GOALS With the Current Generation.
The Pierre Auger Observatory Nicolás G. Busca Fermilab-University of Chicago FNAL User’s Meeting, May 2006.
Jamie Holder School of Physics and Astronomy, University of Leeds, U.K Increasing the Collection Area for IACTs at High Energies Future of Gamma Ray Astronomy.
Gus Sinnis HAWC Review December 2007 Milagro a TeV Gamma-Ray Observatory Gus Sinnis Los Alamos National Laboratory.
A Search for Point Sources of High Energy Neutrinos with AMANDA-B10 Scott Young, for the AMANDA collaboration UC-Irvine PhD Thesis:
Gus Sinnis Los Alamos National Laboratory EAS Arrays in the GLAST Era.
The Milagro Gamma-Ray Observatory By Timothy Willett CROP: Roncalli Division.
HAWC Gus Sinnis VHE Workshop UCLA October, 2005 HAWC: A Next Generation Wide-Field VHE Gamma-Ray Telescope.
The Milagro Gamma-Ray Observatory Milagro is a water Cherenkov extensive air shower (EAS) detector located near Los Alamos, NM at 2630m above sea level,
On A Large Array Of Midsized Telescopes Stephen Fegan Vladimir Vassiliev UCLA.
HAWC: A Next Generation All-Sky VHE Gamma-Ray Telescope.
The ANTARES Neutrino Telescope Mieke Bouwhuis 27/03/2006.
Special Issues on Neutrino Telescopy Apostolos G. Tsirigotis Hellenic Open University School of Science & Technology Particle and Astroparticle Physics.
Julie McEnery GLAST Science Lunch Milagro: A Wide Field of View Gamma-Ray Telescope Julie McEnery.
Alexander Kappes UW-Madison 4 th TeVPA Workshop, Beijing (China) Sep. 24 – 28, 2008 The Hunt for the Sources of the Galactic Cosmic Rays — A multi-messenger.
22 February 2006 Quo Vadis ? Wide Field Imaging A Wide Angle Very Low Threshold Air Cherenkov Imaging Telescope Razmick Mirzoyan MPI Munich, Germany.
High Energy Astrophysics with the High Altitude Water Cherenkov Experiment John Pretz – Los Alamos National Lab International Astronomical Union Meeting.
Gus Sinnis CTA Workshop, Paris, March 2007 Synoptic TeV Telescopes: Recent Results & Future Plans Gus Sinnis Los Alamos National Laboratory.
MiniHAWC Jordan Goodman Beijing – June 2006 Jordan Goodman University of Maryland mini- High Altitude Water Cherenkov experiment  miniHAWC.
Gus Sinnis RICAP, Rome June 2007 High Altitude Water Cherenkov Telescope  Gus Sinnis Los Alamos National Laboratory for the HAWC Collaboration.
Milagro Gus Sinnis Milagro NSF Review July 18-19, 2005 Milagro: A Synoptic VHE Gamma-Ray Telescope Gus Sinnis Los Alamos National Laboratory.
X.-X. Li, H.-H. He, F.-R. Zhu, S.-Z. Chen on behalf of the ARGO-YBJ collaboration Institute of High Energy Physics Nanjing GRB Conference,Nanjing,
High Energy Particle Astrophysics PRC-US Collaboration Summary Report Gus Sinnis David Kieda Gus Sinnis Hu Hongbo Jordan Goodman Min Zha.
Moriond 2001Jordan GoodmanMilagro Collaboration The Milagro Gamma Ray Observatory The Physics of Milagro Milagrito –Mrk 501 –GRB a Milagro –Description.
Milagro Status Report - October October 1998 The Milagro Project Physics Goals Overall Design Milagrisimo - Milagrito - Milagro Comparison of Milagro.
Atmospheric shower simulation studies with CORSIKA Physics Department Atreidis George ARISTOTLE UNIVERSITY OF THESSALONIKI.
Gus Sinnis Asilomar Meeting 11/16/2003 The Next Generation All-Sky VHE Gamma-Ray Telescope.
HAWC Sensitivity Andrew Smith April 20-21,2007 Collaboration Meeting.
HAWC Andrew Smith - University of Maryland TeV Astrophysics II, August 28,2006 High Altitude Water Cherenkov experiment  HAWC Andrew Smith, University.
Multi-TeV  -ray Astronomy with GRAPES-3 Pravata K Mohanty On behalf of the GRAPE-3 collaboration Tata Institute of Fundamental Research, Mumbai Workshop.
XXXI International Cosmic Ray Conference, ICRC 2009 Lodz, Poland, July 7-15, 2009 Time structure of the Extensive Air Shower front with the ARGO-YBJ experiment.
Gamma-Ray Astronomy with the ARGO-YBJ experiment G. Di Sciascio INFN – Sez. Roma “TorVergata” On behalf of ARGO-YBJ Collaboration 5th AGILE Workshop 2008.
A. Smith UMD, April 20-21, 2007 Milagro collaboration meeting The Hidden Potential of the “Gamma’’ Data. The Milagro Gamma-Hadron separation is bases on.
Hadronic interaction studies with the ARGO-YBJ experiment (5,800 m 2 ) 10 Pads (56 x 62 cm 2 ) for each RPC 8 Strips (6.5 x 62 cm 2 ) for each Pad ( 
The HAWC Gamma-Ray Observatory Gus Sinnis Los Alamos National Laboratory for the HAWC Collaboration LHAASO Workshop - Beijing, China February 17, 2011.
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.
1st page of proposal with 2 pictures and institution list 1.
Hybrid measurement of CR light component spectrum by using ARGO-YBJ and WFCTA Shoushan Zhang on behalf of LHAASO collaboration and ARGO-YBJ collaboration.
LHAASO-WCDA Design & Performance Zhiguo Yao for the LHAASO Collaboration IHEP, Beijing 2011/08/17.
EAS Time Structures with ARGO-YBJ experiment 1 - INFN-CNAF, Bologna, Italy 2 - Università del Salento and INFN Lecce, Italy A.K Calabrese Melcarne 1, G.Marsella.
Temporal and spatial structure of the Extensive Air Shower front with the ARGO- YBJ experiment 1 - INFN-CNAF, Bologna, Italy 2 - Università del Salento.
A Future All-Sky High Duty Cycle VHE Gamma Ray Detector Gus Sinnis/Los Alamos with A. Smith/UMd J. McEnery/GSFC.
LAWCA for Air Shower Detection at High Altitude IHEP, Beijing Zhiguo Yao VCI, 11-15/02/2013.
June 6, 2006 CALOR 2006 E. Hays University of Chicago / Argonne National Lab VERITAS Imaging Calorimetry at Very High Energies.
Comparison of different km3 designs using Antares tools Three kinds of detector geometry Incoming muons within TeV energy range Detector efficiency.
Aous Abdo Ground-based Gamma-ray Astronomy: Towards the Future. Santa Fe, NM May 11–12, 2006 Detection of Tev  -rays from the Cygnus Region with Milagro.
Z. Cao, H.H. He, J.L. Liu, M. Zha Y. Zhang The 2 nd workshop of air shower detection at high altitude.
Introduction Active galactic nuclei (AGN) are among the most interesting sources of gamma-rays. At the highest energies, blazars are the most luminous.
Detecting Air Showers on the Ground
Jordan Goodman TeV III Venice August 2007 HAWC - A Wide-Field Gamma-Ray Telescope Jordan A. Goodman University of Maryland.
Milagro at Tibet Gus Sinnis LANL/P-23. Challenge and Opportunity Milagro will run for ~2 more years (or less) No viable candidate to replace Milagro on.
Prospects of Identifying the Sources of the Galactic Cosmic Rays with IceCube Alexander Kappes Francis Halzen Aongus O’Murchadha University Wisconsin-Madison.
The Large High Altitude Air Shower Observatory LHAASO.
Gus Sinnis RICAP, Rome June 2007 The Milagro Observatory: Recent Results & Future Plans Gus Sinnis Los Alamos National Laboratory for the Milagro Collaboration.
Shoushan Zhang, ARGO-YBJ Collaboration and LHAASO Collaboration 4 th Workshop on Air Shower Detection at High Altitude Napoli 31/01-01/ IHEP (Institute.
1 Cosmic Ray Physics with IceTop and IceCube Serap Tilav University of Delaware for The IceCube Collaboration ISVHECRI2010 June 28 - July 2, 2010 Fermilab.
32 nd ICRC –Beijing – August 11-18, 2011 Silvia Vernetto IFSI-INAF Torino, ITALY On behalf of the ARGO-YBJ collaboration Observation of MGRO J with.
A TeV-gamma ray observatory implemented with water Cherenkov array at YBJ Huihai He, IHEP, CAS 2013/2/1 LAWCA (Large Area Water Cherenkov Array)
Downgoing Muons in the IceCube experiment: Final presentation for Phys 735, Particle, Prof. Sridhara Dasu L.Gladstone 2008 Dec 3.
On behalf of the ARGO-YBJ collaboration
Searching for VHE Gamma-Ray Bursts with Milagro
Capability of Extended Air Shower Arrays for Gamma-Ray Astronomy
LHAASO-WCDA: Design & Performance
The Status of the ARGO Experiment at YBJ
HAWC Science Survey of 2p sr up to 100 TeV energies Extended Sources
Estimation of Sensitivity to Gamma Ray point Sources above 30TeV
The Aperture and Precision of the Auger Observatory
"Physics and astronomy results with the ARGO-YBJ experiment"
Presentation transcript:

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith mini- High Altitude Water Cherenkov experiment e   145 meters 4 meters  Andrew Smith University of Maryland

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith What is miniHAWC? Milagro – Existing water Cherenkov all-sky gamma-ray observatory. HAWC – A “science” driven effort to construct an all-sky observatory with point source sensitivity of the Whipple 10m. miniHAWC – Demonstrate HAWC technology at low cost with Milagro PMTs/instrumentation.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith What is the Sensitivity of miniHAWC? Answer: ~15x Milagro. 1y  ~60mCrab source at 5  Interpretation 1: Designers of Milagro are Stupid. Interpretation 2: Designers of miniHAWC are Smart. Designers of Milagro = Designers of miniHAWC Interpretation 3: Designers of Milagro/miniHAWC were naive, but have wised up.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Critical Variables Size – Bigger is better until you reach sqrt(A) regime. Photocathode Density – More is better until you detect all the particles. Altitude – Higher is better until you can’t breathe. Diminishing returns. Tools: PMTs (8” Hamamatsu), Water, black and white materials.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Detector Layout Milagro: 450 PMT (25x18) shallow (1.4m) layer 273 PMT (19x13) deep (5.5m) layer 175 PMT outriggers Instrumented Area: ~40,000m 2 PMT spacing: 2.8m Shallow Area:3500m 2 Deep Area:2200m 2 HAWC: 5625 or PMTs (75x75x1,2) Single layer at 4m depth or 2 layers at Milagro depths Instrumented Area: 90,000m 2 PMT spacing: 4.0m Shallow Area:90,000m 2 Deep Area:90,000m 2 miniHAWC: 841 PMTs (29x29) 5.0m spacing Single layer with 4m depth Instrumented Area: 90,000m 2 PMT spacing: 4.0m Shallow Area:90,000m 2 Deep Area:90,000m 2

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Equipment Milagro DAQ: –898 8” Hamamatsu PMTs –Single data/HV cable ~150m length –Custom front end boards. Analog to level crossing conversion. (Amplitude through time over threshold.) –FASTBUS TDC –VME – FASTBUS interface with VME readout –2000Hz maximum readout with ave multiplicity ~20-30%

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith How do you make an EAS array more sensitive to gamma-ray sources? Energy Threshold –Altitude –Big, hermetic, sensitive Angular Resolution –Big  Lever Arm gamma/hadron Separation –Must detect penetrating particles Sensitivity increase is the product of the improvement made in each category.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith 4500m 2600m Difference between 2600m (Milagro) and 4500m (Tibet): ~ 6x number of particles ~ 2x lower energy threshold Altitude

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Hadron induced cosmic ray showers contain 5-20x more energy in penetrating  +/- and hadrons than EM particles. High P t hadronic interactions lead to wide lateral distributions. Need mass! Need large Area! Muon/hadron Detection HAWC miniHAWC Milagro

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith High Altitude Detector w/o  /hadron separation ARGO: ~6000m 2 RPC detector. Reported at ICRC expect sensitivity of 8-13  /year on the Crab. Milagro currently achieves ~8  /year on the Crab.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Curtains A high altitude version of Milagro would trigger at >10kHz. Need to control spurious triggers due to single muons. Install curtains to optically isolate the the PMTs.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Simulation Strategy Use Milagro Simulation/Reconstruction software. Use observed Milagro crab signal to anchor simulations to reality.  Shared systematics with Milagro. Use new  /hadron discrimination variable for HAWC/miniHAWC that excludes the core location. C Milagro = (nPMTs above 2 PE)/(Max “muon layer” hit) C miniHAWC = (nPMTs above 2 PE)/(Max “muon layer” hit > 20m from core) As an illustration, consider 2 trigger threshold: 50 PMTs, 200 PMTs.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith  = ~0.4 deg  = ~0.25 deg Angular Resolution  /hadron Separation Cut: nTop/cxPE>5.0 Eff  = 34% Eff CR= 3% Cut: nTop/cxPE>5.0 Eff  = 56% Eff CR= 1.5%

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Triggering with Curtains Multiplicity trigger at ~80 PMTs gives same trigger rate as Milagro at 50 PMTs Much higher Gamma area.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Effective Area Detector size

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Energy (Crab Spectrum, nTop/cxPE>5.0.,  <30 O ) Significance from Crab Transit (~5 hr) 4  Crab signif/year80  5  point source sensitivity reach ~60mCrab of 1 year survey Energy Resolution~30% above median Angular Resoultion0.25 O O S/B (hard cuts) ~ 1:1 for Crab Typical day 20 excess on 25 bkg Q(Milagro -> miniHAWC) = 15! Single layer doesn't limit sensitivity miniHAWC Sensitivity

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Curtains Test in Milagro

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Site –High Altitude. –Power –Internet –Don’t need darkness or good weather… –YBJ very interested. –Chinese don’t have money for site prep. (ARGO) –Investigating a site in Mexico.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Cost - Detector Elements Pond ( M$) Black Liner Material $1/m 2 ) Pump/Recirculation System. (~$200k$) PMTs – Reuse with base and encapsulation w/ new connectors. Cables – Purchase new. (~100$k) Front End Electronics – keep as is. TDC and DAQ –2kHz DAQ keep current electronics –Faster  VME TDCs (~200$k) Online computing – A few computers can reconstruct in real time. (~10$k) Building – Assemble functional DAQ in a trailer and ship to site. (~200$k) Internet Access – Live with slow internet if necessary. Need prompt alert capability.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Issues – The Good/Bad Simple Analysis- Event weighting could increase sensitivity further. In Milagro Q=1.6. Can reconstruct showers down to 20 PMTs if we could trigger at 6kHz. Site. Calibration. Noise. Milagro in 1.4y  ~8  /y

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Summary 15x Sensitvity increase over Milagro ~3x from Altitude,Area ~3x from  /hadron separation ~1.5x from Angular resolution ~60mCrab sensitivity (5  in 1year) Mostly proven technology –Leverage $1.5M investment in Milagro equipment –Could construct rapidly if site available.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith An Ideal Air Shower Gamma-Ray Detector: 1) Large Physical Area Collection Area Contain Core Sample Lateral Tails 2) High Efficiency for 20 MeV  Continuous Detector Efficient   e Converter 3) Calorimetry Hadron/Muon Identification 4) Altitude ~40gm/cm 2 increase in altitude  double ground level particles. Lowers threshold.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith 1) Large Physical Area (Diagram Showing Shower Curvature) Core position reconstruction required for accurate angle reconstruction. --> Core must be contained within detector --> Effective area <~ Physical Area --> 10 4 to 10 5 m 2 detector required to rival area of IACTs --> Long lever arm for angle reconstruction. Shower front is curved. Without core position: Pointing error dominated by systematics ==>  PSF >~ 0.7 O

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith 2) High Efficiency for detection of 20MeV Gamma-Rays In extended air showers  's out number e +/- by 5-10 to 1. Mean energy of EAS  's is ~20 MeV. ( not strongly correlated with primary VHE  energy.) Plot showing spectrum of showering particles Plot Showing de/dx for electrons.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith HAWC layout 75x75 grid of 8” PMTs - in 2 layers (depth =2m,6m, separation = 4m) Angle reconstruction with top layer. Calorimetry with bottom layer Opaque “curtains” separate PMT cells. Eliminate “cross talk” between counter. Limits trigger rate compared to Milagro

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith How does the HAWC design measure up? 1) Size: – 300mx300m = 90,000 m 2 2) Efficiency: Water acts a both conversion medium and radiator. ~1 PE/25 MeV 3) Calorimetry: Deep (~15Xo) PMT layer for Muon/Hadron rejection. 4) Altitude: Select optimal site.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Simulation Strategy Simulate various HAWC geometries at 2 altitudes. Compare results with Milagro. (Milagro sensitivity verified by observations of the Crab.) 2 altitudes considered: 4500m ( ~Tibet Lab altitude) 5200m ( ~Atacama Plateau) 2 sets of cuts considered: Std - 50 PMT multiplicity cut Hard PMT multiplicity cut  = ~0.4 deg  = ~0.25 deg

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Gamma-Hadron Separation: Remove events with one or more large hits away from the core ---> muon/hadrons in lateral tails ---> “cxPE” is largest bottom layer hit with R core >10m ---> “nTop” is number of PMTs hit in top layer Cut: nTop/cxPE>10.0 Eff  = 40% Eff CR= 5% Cut nTop/cxPE>10.0 Eff g = 65% Eff CR= 2%

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Energy of reconstructed events (Crab Spectrum) nTop/cxPE>10.,  <30 O Altitude = 4500m Altitude = 5200m Threshold Lower at zenith.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Point Source Sensitivity of HAWC: Altitude5200m4500m Crab Transit (~4 hr) 25  10  Median Energy Time to 5  10min60min 5  point source sensitivity reach 10mCrab25mCrab of 1 year survey Energy Resolution~30% above median ~1/4 sensitivity of HESS (40  /hr) with >1000x the exposure!

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith miniHAWC: HAWC is a potentially large complex project. Consider a another possibility, the relocation of the Milagro apparatus to an optimized pond located at a high altitude site. Milagro owns ~900 8” Hamamatsu PMTs and a DAQ capable of 2000Hz readout. --> Single layer consisting of a 29x29 Grid of PMTs with 5m separation (150mx150m pond) and 4m depth. --> Utilize same reconstruction and  /hadron separation methods as HAWC. --> Simulation altitude 4500m.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Summary: Current EAS arrays are not detecting/utilizing the “whole” shower. Huge improvements in  /hadron separation possible. Excellent angular resolution possible. miniHAWC/HAWC could survey the entire northern or southern sky to a sensitivity of ~60mCrab/10mCrab. (conservative estimates) Limiting detector to a single layer doesn't seem to reduce sensitivity. Could reduce cost of HAWC instrumentation by factor of ~2-3 Wide field of view and high duty cycle: Surveys Prompt VHE GRB emission? AGN monitor. Ideal for study of diffuse/extended sources. ???

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith The Diffuse Galactic Plane in miniHAWC and HAWC Use Neutral H map to trace out VHE Gamma-Ray flux. Normalize to Milagro observed TeV diffuse emission from the Galactic plane.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith Conclusions Milagro and other air-shower arrays play an important and complementary roll in VHE astronomy. –Survey –GRBs –Extended/Diffuse Sources –Monitoring Variable Sources –Solar Activity Monitoring –Water Cherenkov Method has not been exploited efficently –Design improbments (Size, Altitude, …) lead to much better than sqrt(N) sensitivity improvents.

October 20-21, 2005 “Towards the Future” Workshop Andrew Smith

1) Size: – 150m x 150m = 22,500 m**2 2) Efficiency: Water acts a both conversion medium and radiator (Cherenkov) ~1 PE/40 MeV 3) Calorimetry: Deep (~15Xo) PMT layer for Muon/Hadron rejection. 4) Altitude: Select an optimal site.