GALACTIC PHYSICS WITH CTA
Ryan C. G. Chaves1 for the the CTA Consortium
1CNRS/IN2P3 / Univ. Montpellier, France
GALACTIC PHYSICS WITH CTA Ryan C. G. Chaves 1 for the the CTA - - PowerPoint PPT Presentation
GALACTIC PHYSICS WITH CTA Ryan C. G. Chaves 1 for the the CTA Consortium 1 CNRS/IN2P3 / Univ. Montpellier, France THE NEXT GENERATION: CTA The Future of Research on Cosmic Gamma Rays Galactic Physics with CTA, August 2015 2 GALACTIC
Ryan C. G. Chaves1 for the the CTA Consortium
1CNRS/IN2P3 / Univ. Montpellier, France
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015 2
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015 3
Understanding the origin and role of relativistic cosmic particles
What are the sites of high-energy particle acceleration in the Galaxy? What are the mechanisms for cosmic particle acceleration? What role do accelerated particles play in feedback on star formation?
Probing extreme environments
What physical processes are at work close to neutron stars and black holes? What are the characteristics of relativistic jets, winds, and explosions?
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015 4
Dubus+ (CTA) 13
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015 5
Credit: R. Gendler
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015 6
A unique target to study extreme Galactic-type VHE sources & difguse emission (CRs) Face-on satellite galaxy:
no distance ambiguity Very active:
Milky Way
Potential pointing pattern
N.B. Advantage of large CTA FoV
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015 7
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The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015 8
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atomic gas contours
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10 The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
11 The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
Estimated calorimetric gamma-ray flux Estimated CTA sensitivity Current detections
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CTA Survey
13 The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
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Deil, Chaves+ (H.E.S.S.) 15
15 The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
First 2 years: ~2–4 mCrab 10-yr program
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Increase population of known Galactic VHE sources x 3–9+ Discover new VHE source classes and unexpected phenomena Search for Galatic CR PeVatrons Measure large-scale difguse emission Detect new -ray binaries & other variable or transient sources Provide fjrst-look science data to other KSPs & General Observers Produce a multi-purpose legacy dataset to MWL community
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
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Increase population of known Galactic VHE sources x 3–9++
Renaud+09
T A R G E T R A N G E
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
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Discover new VHE source classes and unexpected phenomena
Deil, Chaves+ (H.E.S.S.) 15
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
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Search for Galatic CR PeVatrons
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
CTA South SST s further improve multi-T eV sensitivity + Access to inner Galaxy
20 The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
Source populations modeled:
eVCat) Expected difguse emission: Both IC & π0 components (GALPROP) Energy range: 1-10 T eV ctools open-source software with latest IRFs for North & South arrays Actual GPS observation scheme (1620 h) Most realistic simulations to date & work on-going
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The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
Knoedlseder+ (CTA)
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Where & how in the Galaxy are CRs accelerated up to PeV energies? What is the distribution of PeVatrons in the Galaxy? Are we sitting in a particular location of the Galaxy, or is there a uniform CR sea within the whole Galaxy (understanding diffusion by observing gamma-ray accelerators and their surroundings)? Do young shell-type SNRs accelerate hadronic CRs up to PeV energies? If so, up to which energies, and how effective is this acceleration (probing the theory of non-linear DSA)?
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
24 The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
O n e w a y t
e t t
R k n e e ( ~ 3 P e V ) e n e r g i e s , q u i t e s p e c i fj c : Y
n g , f a s t ( 2 , k m s
) S N R s h
k i n d e n s e w i n d ( C S M ) f r
a T y p e I I S N & R S G p r
e n i t
e . g . 3 3
r
d C a s A , b u t = 2 . 6 ± . 2 Г
s t a t
± . 2
s y s t
O t h e r h i s t
i c a l S N R s a r e c h a l l e n g i n g a s w e l l , c . f . u p d a t e d T y c h
S N I a ) s p e c t r u m f r
V E R I T A S ( = 1 . 9 5 ± . 5 1 Г
s t a t
± . 3
s y s t
→ = 2 . 9 2 ± . 4 1 Г
s t a t
) A r e P e V a t r
s s h
t l i v e d ? M H D i n s t a b i l i t y q u e n c h e d a f t e r ~ 1 y r s ( ~ a g e R X J 1 7 1 3 ) , e . g . S c h u r e & B e l l 2 1 3 E
m a x
~ P e V f
l y ~ 1 y r s
l e s s O b s e r v a t i
s t r a t e g y f
C h e r e n k
t e l e s c
e s ? H i d d e n i n t h e e x i s t i n g d a t a b u t c
f u s e d /
s c u r e d ? J u s t n e e d m
e s t a t i s t i c s / b e t t e r s e n s i t i v i t y a t m u l t i
e V E ? N
l
i n g a t t h e r i g h t
j e c t s , b i a s e d b y w e l l
n
n S N R s ? M
e c u l a r c l
d s ?
25 The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
GPS ideal strategy to identify PeVatron candidates
along entire plane
hundreds of T eV
source confusion
Adapted from Carrigan, Chaves+ (H.E.S.S.) 13
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Specifjcally, candidates should exhibit:
eV
de Oñ a Wilhelmi+ (CTA)
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Solid lines: = 2.0 Dashed lines: = 2.2
CTA simulations
de Oñ a Wilhelmi+ (CTA)
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Deeper obs. (+50 h min.) of most prominent -ray SNR T
hadronic acceleration e.g. through precision imaging of shell morphology T
molecular environment (e.g. Gabici & Aharonian 07) Leveraging next-gen PSF to better match gas studies
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Nakamori+ (CTA) 15
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If leptonic component dominant, search for hidden hadronic component
Nakamori+ (CTA) 15
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Abramowski+ (H.E.S.S.) 15
50% Lradio
Not quite VHE detection ~5 σ X-rays:
Abramowski+ (H.E.S.S.) 14
Pulsar has largest known Edot ~ 4.8 × 1038 erg s-1
Abramowski+ (H.E.S.S.) 14
Largest SFR in Local Group Largest X-ray synchrotro n shell known (47 pc) 10x as bright as SN 1006 Powered by
Abramowski+ (H.E.S.S.) 14
ldiff = sqrt(2 D t) < ~47 pc D(10 TeV) < ~3.3 × 1026 (t/106 yr)−1 cm2 s−1 2-3 orders lower than ~Galactic requires MFA / B turbulence still open question: leptonic vs. hadronic
High shock speed High ambient density Hadronic? Upper limit
now, but more
s planned & emission predicted to increase
Predicted: ∼8 × 10−14 cm−2 s−1 in 2013 ∼2.5 × 10−14 cm−2 s−1 in 2010 F (> 1 TeV) < 5 × 10−14 cm−2 s−1 99% CL during 2003-2012
Abramowski+ (H.E.S.S.) 14
Abramowski+ (H.E.S.S.) 14
Abramowski+ (H.E.S.S.) 14
Still lack statistics to disentangle? Not sensitivity limited in latitude? Roughly fjts plausible counterpart distributions
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
FYI: CTA GPS by ~2022
The Future of Research on Cosmic Gamma Rays – Galactic Physics with CTA, August 2015
Triple the exposure Improved gamma-hadron separation Improved angular resolution
X-rays (XMM-Newton) convolved with H.E.S.S. PSF
Are cosmic rays escaping the shell and interacting with molecular clouds? i.e. is there TeV emission beyond the shell?
around ~10 TeV ( not a → PeVatron)