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VHE Gamma-Ray Astronomy via Particle Detection at the

Ground Level

Or

A biased review of VHE Gamm-Ray Survey Instruments

Petra Huentemeyer

petra@mtu.edu

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The Players:

EAS Arrays

Particle Sampling Gamma Rays

Tibet AS-γ 1990-present

ARGO 2007-2014 Milagro

2000-2008

HAWC

2013 - present

LHAASO 2018/19-

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Altitude Gamma-Ray Detectors

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EAS Sampling Arrays 3 Main Features

• Hight Duty Cycle Transients

• Wide Field of View

Extended and Large Scale Emission

• Good Sensitivity, Angular & Energy Resolution above 10s of TeV

Highest Energy Accelerators

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Northern TeV (Gamma-Ray) Surveys

B. Bartoli et al. [ARGO-YBJ Collaboration], ApJ 779, 27 (2013) Science314:439-443,2006

Tibet AS-γ ARGO

11 candidate sources, median energy ~ 1 TeV

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Another Survey: Milagro 2000-2008

Crab at 17σ in 8 years.

Astrophys.J.664:L91-L94,2007

8 candidate sources, median energy ~ 20 TeV

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Latest Survey: HAWC 11/2014-04/2018

Crab at 17σ in 8 years.

>39 candidate sources, pivot energy ~ 7 TeV

The Astrophysical Journal, Volume 843, Issue 1, article id. 40, 21 pp. (2017)

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Galactic Plane Observations over the Years

Preliminary

Milagro (2000-2008)

HAWC Pass 1 (2013-2014, partial array, candidates

HAWC Pass 4 (11/2014-04/2018)

Milagro was located near Los Alamos, New Mexico

different sensitivity by declination along Galactic plane.

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The Other Hillas Parameter: S(nn) or Rho (nnn)

Experimental Astronomy, Volume 44, Issue 1, pp.1-9

NKG Fit

Tibet AS-γ: S50 HAWC: S40

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HAWC High Energy Catalog

> 56 TeV

> 100 TeV

7 candidate sources, energy > 56 TeV, energy spectra forth coming

Acceleration mechanisms: hadronic or leptonic?

Correlation with neutrinos?

Prospects for testing Lorentz Invariance Violation.

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Addition Development: Energy Estimation via ANN

• Toolkit for Multivariat Analysis (TMVA)

1

• Input variable chosen to quantify:

- Core position

- Zenith angle

- Signal at core

- Radial distribution, annuli (show age)

- Energy deposited in detector

- Fraction of ground energy landing in the detector

• 479 free parameters (weights) determined by training on

Gamma-Ray Monte Carlo

1http://tmva.sourceforge.net/

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Energy Estimation via ANN

PMT Hit Occupancy NN

“fhit

NN Energy better correlated with MC truth than previously used variable (fraction of PMT hits)

As for S40 provides a way to determine energies beyond 100 TeV with considerably better precision (~ 16 % at highest energies)

Stay tuned for spectra (after systematics have been sorted out)

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Multisource Fitting Example:

Hunting for CR Acceleration in SFRs

The Astrophysical Journal, Volume 753, Issue 2, article id. 159, 8 pp. (2012)

The Astrophysical Journal, Volume 790, Issue 2, article id. 152, 5 pp. (2014)

Milagro

Argo

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Multisource Fitting Example:

Hunting for CR Acceleration in SFRs

with HAWC

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Model Building I

• Fermi detection at GeV (Ackermann et al., Science 334, 2011)

- Extended (50 pc) diffuse HE gamma-ray source

- 'Cocoon' of freshly accelerated CRs - Accelerator:

‣ γ Cygni SNR?

‣ OB2 association (star-forming region)?

- Modeled as symmetric Gaussian

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Model Building II

• Extended VHE gamma-ray source (E.Aliu et al. Apj 783, 2014)

• Associated with PWN of PSR J2032+413

• Long-period binary system:

- Period of 50 years (Ng et al, 2017).

- Periastron in November 2017.

• Modeled as asymmetric Gaussian, 


PL spectrum (R. Bird et at, ICRC 2017).

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Model Building III

• Extended (0.1 deg) VHE gamma-ray source (E. Aliu et al., ApJ 770, 93, 2013)

• Additional extended disk component
 (Strysz et al., ICRC 2017).

• SNR G78.2+2.1 of PSR J2021+4026

• Offset between HAWC & VTS centroids.

• Modeled as PS (morphological studies
 ongoing), PL spectrum.

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Combined Model

- =

HAWC Preliminary

HAWC

HAWC Preliminary HAWC Preliminary

Map on the left has PWN &

Gamma-Cygni subtracted

Blue Contours are Fermi-LAT

Energy spectrum is forthcoming, challenge:

identification of the VHE

energy emission, from PWN or from Cocoon

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Multisource Fit Approach was used in

HAWC Analysis of micro quasar SS43

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Physics Model & Templates: Example Geminga

Abeysekara et al. (2017): Science, 358, 911

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Discovery Potential:

Hiding in Plane Sight

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Discovery Potential:

Hiding in Plane Sight

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Multi-Instrument Fits:

Example Gamma-Cygni

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Outriggers & Further Analysis Improvements

4x sensitivity above 50 TeV:

Better shower core fit

Shower containment (better energy resolution)

Current low-energy (small

event) angle reconstruction is limited by noise.

The “noise” in HAWC is

almost entirely due to small non-triggering showers.

New “Multi-Plane Fitter”

identifies and isolates sub- showers within each event instead of assuming all hits are from a single shower.

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Complementarity LHAASO & HAWC

HAWC and LHAASO are at about the same latitude (28°N) but opposite sides of the globe. Together they minimize the survey gap of the Northern hemisphere!

Gravitational Waves

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The EAS Sampling Future:

• Factor of 4 increase SGSO

in sensitivity between ALMA (5000 m a.s.l.) and HAWC (4100 m a.s.l.) altitude

• Lower energy threshold

• Discovering rate transient events requires full sky

coverage (e.g. GRBs

& GW)

• TeV source finder for CTA South

Cosmic Rays

• Spectrum (CR + electrons)

• Mass composition + interaction model studies

• Anisotropies (CR + electrons)

PRELIMINARY

Energy (GeV)

104 105 106 107 108

]1.6 GeV-1 sr-1 s-2 [m2.6Flux x E

102 103 104

Horandel (p+He) CREAM (p+He) ARGO-YBJ analog All Particle ICRC15 ID366 ARGO-YBJ analog All Particle ICRC15 ID382 ARGO-YBJ analog All Particle (Bayes) ARGO-YBJ 2015 digital (p+He) PRD91 (2015) 112017 ARGO-YBJ analog Bayes (p+He) ARGO/WFCTA hybrid (p+He) PRD92 (2015) 092005 Tibet Array All Particle - QGSJet IceTop 73 All Particle - SIBYLL KASCADE All Particle - QGSJet KASCADE-Grande All Particle - QGSJet TUNKA 25 All Particle HAWC All Particle - arXiv:1710.00890

Galactic particle accelerators

• Pulsars constraining local e+ flux

• Extended sources: Fermi-Bubbles

• Deep survey for Pevatrons

• Monitoring of variable sources

Science with the

Southern Gamma Survey Observatory

Fabian Schüssler on behalf of the SGSO Alliance sgso-alliance.org

The Southern Gamma Survey Observatory (SGSO)

Next generation !-ray observatory

• Wide-FoV particle detector array with ~100% duty-cycle

• High-altitude site on Southern Hemisphere

• Energy range: 100GeV to 100TeV

• Complementary to HAWC/LHAASO and CTA

The SGSO Alliance

• sgso-alliance.org

• Group of (~85} scientists interested in the development of a next generation gamma-ray observatory in the Southern hemisphere

• Various sites and detector designs being studied in parallel

• Prototyping of detector stations in progress

• White paper on the science case in preparation (summary here) Feel free to join the SGSO Alliance at sgso-alliance.org

The Science of SGSO

Physics beyond the SM

• Dark Matter

Galactic Center

dSph: many new candidates

• Lorentz Variance Violation

Reach to the highest energies

RXJ1713.7-3946

Straw man detector: size and fill-factor Pulsars t< 106 yrs

Straw man detector

Potential SGSO site joint with JAMA+CUBIC (near San Antonio de los Cobres, Argentina)

CORSIKA

HAWC: !/h separation, Ω+E resolutions

Fermi-Bubbles at TeV energies

Energy [eV]

10-7 10-5 10-3 10-1 10 103 105 107 109 1011 1013 1015 ] -2 cm -1 [erg sν Fν

10-16 10-15 10-14 10-13 10-12 10-11 10-10

1ES 0229+200 1ES 0347-121 1ES 1101-232 SGSO - 1y SGSO - 5y

Extreme blazars - SED • Daily monitoring of AGNs

long-term LCs for O(10) sources

LC(min) for brightest flares

alerts to the community (e.g. CTA)

Access to Extreme HBLs

• GRBs + Gravitational waves

• High-energy neutrinos

GW170817 (from M.M. Kasliwal et al., Science 2017)

F. Schüssler (H.E.S.S. Collaboration), TeVPA 2018 11 days between IC-170922

and TeV flare of TXS 0506+056

Monitoring the Transient Sky

See dedica

ted poster by H.

Fleischhack

See also

• M. Mostafa et al., On the scientific motivation for a wide field-of-view TeV gamma-ray observatory in the Southern Hemisphere, PoS ICRC2017 (2017) 851.

• H. Schoorlemmer, R. López-Coto and J. Hinton, Baseline Design for a Next Generation Wide-Field-of-View Very-High-Energy Gamma-Ray Observatory, PoS ICRC2017 (2017) 819.

This work was supported by the Programme National des Hautes Energies of CNRS/INSU with INP and IN2P3, co-funded by CEA and CNES

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