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The Spectrum of Markarian 421 Above 100 GeV with STACEE Jennifer Carson UCLA / Stanford Linear Accelerator Center February 2006 100 MeV 1 GeV 10 GeV 100 GeV 1 TeV 10 TeV 10 MeV 1 MeV Space-based Ground-based

The Spectrum of Markarian 421 Above 100 GeV with STACEE

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The Spectrum of Markarian 421 Above 100 GeV with STACEE. Jennifer Carson UCLA / Stanford Linear Accelerator Center February 2006. Space-based. 10 MeV. 100 MeV. 10 GeV. 100 GeV. 10 TeV. 1 GeV. 1 TeV. 1 MeV. Ground-based. Outline. - PowerPoint PPT Presentation

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Page 1: The Spectrum of Markarian 421  Above 100 GeV with STACEE

The Spectrum of Markarian 421 Above 100 GeV with STACEE

Jennifer CarsonUCLA / Stanford Linear Accelerator Center

February 2006

100 MeV

1 GeV 10GeV

100GeV

1 TeV 10 TeV

10 MeV

1 MeV

Space-based

Ground-based

Page 2: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Outline

I. Science goal for -ray detections from active galaxies• Understanding particle acceleration

II. Brief overview of VHE gamma-ray astronomy

III. Ground-based detection techniques• Atmospheric Cherenkov technique• Imaging vs. wavefront sampling

IV. STACEE

V. Markarian 421• First STACEE spectrum• Detection of high-energy peak?

VI. Prospects for the future

Page 3: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Blazars

• bright core

• 3% optical

polarization

• strong multi-wavelength

variability

Radio-loud AGN viewed at small angles to the jet axis

Page 4: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Blazars

• bright core

• 3% optical

polarization

• strong multi-wavelength

variability

• Double-peaked SED:

synchrotron emission + ?

Radio-loud AGN viewed at small angles to the jet axis

What physical processes produce the high-energy emission?

Maraschi et al. 1994

1 eV (IR) 1 keV (X-ray) 1 MeV10-3 eV (radio) 1 GeV

synchrotron

?

Page 5: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Blazar High-Energy Emission ModelsIs the beam particle an e- or a proton?

Page 6: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Blazar High-Energy Emission Models

Leptonic models:• Inverse-Compton scattering off accelerated electrons• Synchrotron self-Compton and/or • External radiation Compton

Is the beam particle an e- or a proton?

Page 7: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Blazar High-Energy Emission Models

Leptonic models:• Inverse-Compton scattering off accelerated electrons• Synchrotron self-Compton and/or • External radiation Compton

Hadronic models:• Accelerated protons• Gamma rays from pion decay or• Synchroton gamma-ray photons

Is the beam particle an e- or a proton?

Page 8: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Blazar High-Energy Emission Models

Leptonic models:• Inverse-Compton scattering off accelerated electrons• Synchrotron self-Compton and/or • External radiation Compton

Hadronic models:• Accelerated protons• Gamma rays from pion decay or• Synchroton gamma-ray photons

Gamma-ray observations around 100 GeV can distinguish between models

Is the beam particle an e- or a proton?

Page 9: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Exploring the Gamma-ray Spectrum

Atm. Cherenkov Single Dish Imaging

Compton Gamma Ray Observatory

100 MeV

1 GeV 10GeV

100GeV

1 TeV 10 TeV

10 MeV

Energy

1 MeV

Atm. Cherenkov Wavefront Sampling

Air shower arrays

GLAST

Atm. Cherenkov Wavefront Sampling

Atm. Cherenkov Imaging Arrays

Pas

tP

rese

nt/F

utur

e

Page 10: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Atmospheric Cherenkov Technique

ray

~ 1.5oe+

e+

e+

e-

e-

e+

Page 11: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Single-dish Imaging Telescopes

ray

~ 1.5o

Whipple 10-meter

Page 12: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Wavefront Sampling Technique

ray

~ 1.5o

Page 13: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Wavefront Sampling Technique

ray

~ 1.5o

Page 14: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Exploring the Gamma-ray Spectrum

Atm. Cherenkov Single Dish Imaging

Compton Gamma Ray Observatory

100 MeV

1 GeV 10GeV

100GeV

1 TeV 10 TeV

10 MeV

Energy

1 MeV

Atm. Cherenkov Wavefront Sampling

Air shower arrays

GLAST

Atm. Cherenkov Wavefront Sampling

Atm. Cherenkov Imaging Arrays

Whipple 10-meter

Pas

tP

rese

nt/F

utur

e

Page 15: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Exploring the Gamma-ray Spectrum

Atm. Cherenkov Single Dish Imaging

100 MeV

1 GeV 10GeV

100GeV

1 TeV 10 TeV

10 MeV

Energy

1 MeV

Atm. Cherenkov Wavefront Sampling

Air shower arrays

GLAST

Atm. Cherenkov Wavefront Sampling

Atm. Cherenkov Imaging Arrays

Whipple 10-meter

STACEE

CELESTE

Page 16: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Exploring the Gamma-ray Spectrum

Atm. Cherenkov Single Dish Imaging

100 MeV

1 GeV 10GeV

100GeV

1 TeV 10 TeV

10 MeV

Energy

1 MeV

Atm. Cherenkov Wavefront Sampling

Air shower arrays

GLAST

Atm. Cherenkov Wavefront Sampling

Atm. Cherenkov Imaging Arrays

Pre

sent

/Fut

ure

STACEE

Page 17: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Exploring the Gamma-ray Spectrum

100 MeV

1 GeV 10GeV

100GeV

1 TeV 10 TeV

10 MeV

Energy

1 MeV

GLAST

Atm. Cherenkov Wavefront Sampling

Atm. Cherenkov Imaging Arrays

HESS

VERITAS

Pre

sent

/Fut

ure

STACEE

Page 18: The Spectrum of Markarian 421  Above 100 GeV with STACEE

The High-Energy Gamma Ray Sky

1995 3 sources

Mrk421

Mrk501

Crab

R.A.OngAug 2005

Pulsar Nebula

SNR

AGN

Other, UNID

(2)(1)

(0) (0)

Page 19: The Spectrum of Markarian 421  Above 100 GeV with STACEE

The High-Energy Gamma Ray Sky

2004 12 sources

Mrk421 H1426

Mrk501

1ES1959

1ES 2344

PKS 2155

Cas A

RXJ 1713

CrabTeV 2032

M87

GC

R.A.OngAug 2005

Pulsar Nebula

SNR

AGN

Other, UNID

(7)(1)

(2) (1,1)

Page 20: The Spectrum of Markarian 421  Above 100 GeV with STACEE

The High-Energy Gamma Ray Sky

2005 31 sources!

Mrk421 H1426

Mrk501

1ES1959

1ES 2344

PKS 2155

Cas A

RXJ 1713

CrabTeV 2032

M87

PKS 2005

PSR B1259

RXJ 0852

MSH 15-52

SNR G0.9

HessJ1303

GC

R.A.OngAug 2005

Pulsar Nebula

SNR

AGN

Other, UNID

H2356

1ES 1218

1ES 1101

LS 5039Vela X

+ 8-15 add. sourcesin galactic plane.

CygnusDiffuse

(11)(4+2)

(3+4) (3,3+1)

Page 21: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Wavefront Sampling DetectorsSTACEE & CELESTE

e+

e+

e+

e-

e-

e+

Cherenkov light intensity on ground energy of gamma ray

Cherenkov pulse arrival times at heliostats direction of source

Page 22: The Spectrum of Markarian 421  Above 100 GeV with STACEE

STACEE

64 heliostats

5 secondary mirrors & 64 PMTs

National Solar Thermal Test FacilityAlbuquerque, NM

Solar Tower Atmospheric Cherenkov Effect Experiment

Page 23: The Spectrum of Markarian 421  Above 100 GeV with STACEE

STACEE

64 heliostats

5 secondary mirrors & 64 PMTs

National Solar Thermal Test FacilityAlbuquerque, NM

Solar Tower Atmospheric Cherenkov Effect Experiment

• PMT rate @ 4 PEs: ~10 MHz

• Two-level trigger system (24 ns window): - cluster: ~10 kHz - array: ~7 Hz

• 1-GHz FADCs digitize each Cherenkov pulse

Page 24: The Spectrum of Markarian 421  Above 100 GeV with STACEE

STACEE Advantages / Disadvantages

• 2-level trigger system good hardware rejection of hadrons

• GHz FADCs pulse shape information

• Large mirror area (6437m2) low energy threshold

Ethresh = 165 GeV

Page 25: The Spectrum of Markarian 421  Above 100 GeV with STACEE

STACEE Advantages / Disadvantages

• 2-level trigger system good hardware rejection of hadrons

• GHz FADCs pulse shape information

• Large mirror area (6437m2) low energy threshold

But…• Limited off-line cosmic ray rejection limited sensitivity: 1.4/hour on the Crab Nebula

• Compare to Whipple sensitivity: 3/hour above 300 GeV

Ethresh = 165 GeV

Page 26: The Spectrum of Markarian 421  Above 100 GeV with STACEE

STACEE Data

Observing Strategy: Equal-time background observations for every source observation (1-hour “pairs”)

Cuts for data quality

Correction for unequal NSB levels

Cosmic ray background rejection

Analysis:

Significance/flux determination

Page 27: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Energy Reconstruction Idea

Utilize two properties of gamma-ray showers:

1. Linear correlation: Cherenkov intensity and gamma-ray energy

2. Uniform intensity over shower area

200 GeV gamma ray 500 GeV proton

Page 28: The Spectrum of Markarian 421  Above 100 GeV with STACEE

New method to find energies of gamma rays from STACEE data:1. Reconstruct Cherenkov light distribution on the ground from PMT charges2. Reconstruct energy from spatial distribution of light

Energy Reconstruction Method

Results:

fractional errors < 10%

energy resolution ~25-35%

Page 29: The Spectrum of Markarian 421  Above 100 GeV with STACEE

STACEE

• Nearby: z = 0.03• First TeV extragalactic source detected (Punch et al. 1992)• Well-studied at all wavelengths except 50-300 GeV• Inverse-Compton scattering is favored• High-energy peak expected around 100 GeV• Only one previous spectral measurement at ~100 GeV (Piron et al. 2003)

Markarian 421

Blazejowski et al. 2005

Krawczynski et al. 2001

log (Energy/eV)

log

(E2 d

N/d

E /

erg

cm-2

s-1)

?

STACEE

Page 30: The Spectrum of Markarian 421  Above 100 GeV with STACEE

STACEE Detection of Mkn 421

Pairwise distribution of

• Observed by STACEE January – May 2004• 9.1 hours on-source + equal time in background observations• Non – Noff = 2843 gamma-ray events• 5.8 detection• 5.52 0.95 gamma rays per minute• Energy threshold ~198 GeV for = 1.8

Eth = 198 GeV = 1.8

Page 31: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Rat

e (p

hoto

ns s

-1 G

eV-1)

Aef

f(E)

(m2 )

Energy (GeV)

Spectral Analysis of Mkn 421

Gamma-ray rate (photons s-1 GeV-1) Effective area (m2)

• Six energy bins between 130 GeV and 2 TeV• Find gamma-ray excess in each bin• Convert to differential flux with effective area curve

Energy (GeV)

Page 32: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Spectral Analysis of Mkn 421

= 1.8 0.3stat

First STACEE spectrum

Page 33: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Spectral Analysis of Mkn 421

= 1.8 0.3stat

First STACEE spectrum

Flat SED

Page 34: The Spectrum of Markarian 421  Above 100 GeV with STACEE

2004 Multiwavelength Campaign

January February March April

TeV

X-ray

PC

A data courtesy of W

. Cui, B

lazejowski et al. 2005

Page 35: The Spectrum of Markarian 421  Above 100 GeV with STACEE

2004 Multiwavelength Campaign

January February March April

TeV

X-ray

STACEEobservations

PC

A data courtesy of W

. Cui, B

lazejowski et al. 2005

• STACEE coverage: 40% of MW nights• ~90% of STACEE data taken during MW nights• STACEE combines low and high flux states

Page 36: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Multiwavelength Results

Blazejow

ski et al. 2005

Page 37: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Multiwavelength Results

STACEE region

Blazejow

ski et al. 2005

Page 38: The Spectrum of Markarian 421  Above 100 GeV with STACEE

STACEE + Whipple Results

Page 39: The Spectrum of Markarian 421  Above 100 GeV with STACEE

STACEE + Whipple Results

Page 40: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Science Interpretation

• STACEE’s first energy bin is ~120 GeV below Whipple’s.

• STACEE result:

is consistent with a flat or rising SED.

suggests that the high-energy peak is above ~200 GeV.

slghtly is inconsistent with most past IC modeling.

• Combined STACEE/Whipple data suggest that the peak is around 200-500 GeV.

• SED peak reflects peak of electron energy distribution.

Page 41: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Prospects for the Future

• STACEE will operate for another year

Air Cherenkov Single Dish Imaging

100 MeV

1 GeV 10GeV

100GeV

1 TeV 10 TeV

10 MeV

Energy

1 MeV

Compton Gamma Ray Observatory

Air Cherenkov Wavefront Sampling

Gamma-ray spectrum

Page 42: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Prospects for the Future

• STACEE will operate for another year

• Imaging arrays coming online, Ethreshold 150 GeV - HESS: 5 Crab detection in 30 seconds! - VERITAS: 2 (of 4) dishes completed

Air Cherenkov Imaging Arrays

100 MeV

1 GeV 10GeV

100GeV

1 TeV 10 TeV

10 MeV

Energy

1 MeV

Compton Gamma Ray Observatory

Air Cherenkov Wavefront Sampling

Gamma-ray spectrum

Page 43: The Spectrum of Markarian 421  Above 100 GeV with STACEE

VHE Experimental World

STACEE

MILAGRO

TIBETARGO-YBJ

PACT

GRAPES

TACTIC

VERITAS

MAGIC

HESS CANGAROO

TIBETMILAGRO

STACEE

TACTIC

Page 44: The Spectrum of Markarian 421  Above 100 GeV with STACEE

Compton Gamma Ray Observatory

Prospects for the Future

100 MeV

1 GeV 10GeV

100GeV

1 TeV 10 TeV

10 MeV

Energy

1 MeV

Air Cherenkov Wavefront Sampling

GLAST

Gamma-ray spectrum

Air Cherenkov Imaging Arrays

• STACEE will operate for another year

• Imaging arrays coming online, Ethreshold 150 GeV - HESS: 5 Crab detection in 30 seconds! - VERITAS: 2 (of 4) dishes completed

• GLAST launch in 2007!

Page 45: The Spectrum of Markarian 421  Above 100 GeV with STACEE

GLAST

• Two instruments: LAT: 20 MeV – >300 GeV GBM: 10 keV – 25 MeV

• LAT energy resolution ~ 10%

• LAT source localization < 0.5’

GLAST Large Area Telescope (LAT)

Burst Monitor (GBM)

Page 46: The Spectrum of Markarian 421  Above 100 GeV with STACEE

EGRET Sources

Page 47: The Spectrum of Markarian 421  Above 100 GeV with STACEE

GLAST Potential

Page 48: The Spectrum of Markarian 421  Above 100 GeV with STACEE

• Gamma-ray observations of AGN are key to understanding particle acceleration in the inner jets

• Many new VHE gamma-ray detectors & detections

• STACEE - “1st-generation” instrument sensitive to ~100 GeV gamma rays - Energy reconstruction is successful - 5.8 detection of Markarian 421 - Preliminary spectrum between 130 GeV and 2 TeV - Second spectrum of Mkn 421 at 100-300 GeV - High-energy peak is above ~200 GeV

• Bright future for gamma-ray astronomy

Conclusions