the radio/gamma connection€¦ · mixing source’ gamma-ray lcs: e.g. source 1 (radio) with...
TRANSCRIPT
cm to short-mm band radio and ! gamma-ray correlated variability ! in Fermi bright blazars
Lars Fuhrmann (Max-Planck-Institut für Radioastronomie, Bonn)
S. Larsson (Stockholm Univ.), J. Chiang (Stanford Univ.), E. Angelakis, V. Pavlidou, I. Nestoras, N. Marchili, T. P.
Krichbaum, C. Fromm, J. A. Zensus (MPIfR)
on behalf of the
F-GAMMA and Fermi/LAT collaborations
100-m Effelsbergcovers the band 2.64 - 43 GHz with a precision of a few percent for monthly sampling of 60 sources
30-m IRAMcovers the band 86 - 250 GHz monthly also for roughly 60 sources
12-m APEX 345 GHz, located in Atacama desert in Chile at an altitude of 5100 m
The radio/gamma connection: !
F-GAMMA program
Fermi-GST γ-ray blazars: broad band monitoring of variability and spectral evolution at cm/mm/sub-mm wavelengths
http://www.mpifr-bonn.mpg.de/div/vlbi/fgamma
Fuhrmann et al. 2007, Angelakis et al. 2008, Fuhrmann et al. in prep.
image by N. Tacken
The radio/gamma-ray connection!Where in the jets are the gamma-rays produced? Timing analysis
radio cm/mm (F-GAMMA program) vs. Fermi-LAT 3.5 yr light curves:
0
5e-08
1e-07
1.5e-07
2e-07
2.5e-07
3e-07
3.5e-07
flux
(E>1
00 M
eV) [
ph c
m-2
s-1]
Fermi LAT
J0854+2006
54800 55000 55200 55400 55600 55800MJD
0
2
4
6
8
10
12
14
flux
dens
ity [J
y]
3mm PV9mm EFF20mm EFF60mm EFF
PRELIMINARY
Fermi-GST
100-m Effelsberg & IRAM 30-m
0
5e-08
1e-07
1.5e-07
2e-07
2.5e-07
3e-07
3.5e-07
flux
(E>1
00 M
eV) [
ph c
m-2
s-1]
Fermi LAT
J0854+2006
54800 55000 55200 55400 55600 55800MJD
0
2
4
6
8
10
12
14
flux
dens
ity [J
y]
3mm PV9mm EFF20mm EFF60mm EFF
PRELIMINARY
-400 -300 -200 -100 0 100 200 300 400LAG [days]
-0.2
-0.1
0
0.1
0.2
0.3
DCC
F
all sources
averaged DCCFs
LAT / 3mm radio
PRELIMINARY
statistical Discrete Cross-Correlation Function analysis:
stacking analysis: averaging over whole sample (58 sources)
relative timing of flares
Aim: study focusing on the possible connection between radio and gamma-ray flares/activity periods in the ~ 3.5 yr long-term light curves of about 60 Fermi-GST detected blazars through a detailed cross-band analysis
Main question: where in the jets are the gamma-rays produced (very close to BH ! or on pc-scales) ? (e.g. Blandford & Levinson 1995, Valtaoja et al. 1992, Jorstad ! et al. 2001, Agudo et al. 2011, Leon-Tavares et al. 2011)!
0
1
2
3
4
5
6
7
54000.0 54500.0 55000.0 55500.0 56000.0
2007.0 2008.0 2009.0 2010.0 2011.0 2012.0 2013.0
Flux
Den
sity
(Jy)
MJD
J0238+1636
F-GAMMA team: Preliminary. Not for publication, distribution or any official use!
eangelakis or lfuhrmann at mpifr.de (F-GAMMA team)
2.64 GHz 4.85 GHz 8.35 GHz
10.45 GHz 14.60 GHz 23.05 GHz 32.00 GHz 42.00 GHz 86.00 GHz
142.33 GHz228.39 GHz
Project overview !The sample and data sets
1) radio bands: F-GAMMA program since Jan. 2007:
3-4.5 yrs of Effelsberg 100-m/IRAM 30-m monthly monitoring data at 10 different frequencies (110, 60, 36, 28, 20, 13, 9, 7, 3, 2 mm) + APEX (0.8 mm)
“the best suitable” 58 1FGL sources (best sampl., frequency & time coverage) sample statistics:
Type # FSRQ 33 BL Lac 17 RG 2 Blazar 5 NLSy1 1 2) Fermi/LAT 3.5 yr monthly light
curves: Aug. 2008 – Dec. 2011
specific time boundaries to best match the radio light curves – start Aug. 15, 2008
RSP pipeline, energy range 0.1 – 300 GeV using power law over that energy range
2FGL sources for ROI, ROI size etc.
0
5
10
15
20
25
30
35
40
45
54000.0 54500.0 55000.0 55500.0 56000.0
2007.0 2008.0 2009.0 2010.0 2011.0 2012.0 2013.0
Flux
Den
sity
(Jy)
MJD
J2253+1608
F-GAMMA team: Preliminary. Not for publication, distribution or any official use!
eangelakis or lfuhrmann at mpifr.de (F-GAMMA team)
2.64 GHz 4.85 GHz 8.35 GHz
10.45 GHz 14.60 GHz 23.05 GHz 32.00 GHz 42.00 GHz 86.00 GHz
142.33 GHz228.39 GHz
Cross-band analysis!The light curves
Examples:
0
5e-07
1e-06
flux
(E>1
00 M
eV) [
ph c
m-2
s-1] Fermi LAT
J0238+1637
54800 55000 55200 55400 55600 55800MJD
1
2
3
4
5
6
7
flux
dens
ity [J
y]
2mm PV3mm PV9mm EFF13mm EFF20mm EFF60mm EFF
PRELIMINARY
0
1e-07
2e-07
3e-07
4e-07
5e-07
6e-07
flux
(E>1
00 M
eV) [
ph c
m-2
s-1] Fermi LAT
J0854+2006
54800 55000 55200 55400 55600 55800MJD
5
10
15flu
x de
nsity
[Jy]
2mm PV3mm PV9mm EFF13mm EFF20mm EFF60mm EFF
PRELIMINARY
Fermi-LAT
F-GAMMA radio
Project overview !Three different approaches
1) statistical Discrete Cross-Correlation Function (DCCF analysis)
[ 2) direct LC analysis: relative timing of flare onsets ]
[ 3) fluxr – fluxγ analysis using simultaneous, monthly fluxes ]
0
2e-07
4e-07
6e-07
8e-07
flux
(E>1
00 M
eV) [
ph c
m-2
s-1]
Fermi LAT
J1159+2914
54800 55000 55200 55400 55600 55800MJD
1
2
3
4
flux
dens
ity [J
y]
2mm PV3mm PV9mm EFF13mm EFF20mm EFF60mm EFF
PRELIMINARY
0
5e-06
1e-05
1.5e-05
2e-05
2.5e-05
flux
(E>1
00 M
eV) [
ph c
m-2
s-1]
Fermi LAT
J2253+1608
54800 55000 55200 55400 55600 55800MJD
0
10
20
30
40
flux
dens
ity [J
y]
2mm PV3mm PV9mm EFF13mm EFF20mm EFF60mm EFF
PRELIMINARY
DCCF analysis!The setup
compute DCCFs for each source: for all gamma-ray – radio (ν, ν = 142, 86….2.6 GHz) combinations following Edelson & Krolik (1988)
caveats: 3.5 yrs – still limited number of events, complicated flare structures (multiple sub-flares), “broad DCCFs”, what correlates?, “monthly smoothing” etc.
determine significances of correlations: test of chance correlations by mixing source’ gamma-ray LCs: e.g. source 1 (radio) with source 2 to N (gamma-ray), find “upper envelop” confidence levels
time lags with uncertainties are estimated by Monte Carlo simulations (Peterson et al. 1998)
apply method to the whole sample plus sub-dividing according to FSRQs, BL Lacs, spectral type, physical parameters etc.
stacking of DCCFs: increasing the significance, study of averaged behavior of the sample
DCCF analysis!First results
3 mm vs Fermi/LAT: examples of single source’ DCCFs
- single source cases often not significant: just a few so far! - often no obvious, simple 1:1 correlation - not yet long enough data trains - conservative upper envelops - dashed lines: significance levels
LAT / 3mm DCCFs
DCCF analysis!First results
3 mm vs. Fermi/LAT: stacking of DCCFs
dashed lines: different confidence levels
DCCF peak > than our confidence levels
averaged over whole sample: we obtain highly significant correlations !
DCCF analysis!First results
radio vs. Fermi/LAT: stacking of DCCFs
all LAT/radio (110 to 2 mm) combinations
DCCF peaks all > than our confidence levels
observers frame rest frame
asymmetry
DCCF analysis!First results
sub-grouping: FSRQs vs. BL Lacs Dependence on physical parameters? e.g. BH masses (MBH):
- MBH estimates for 33 sources - low mass range: < 108.9 - high mass range: > 108.9
stronger DCCF peaks & lower lags for high MBH, e.g. FSRQs:
<lag>3mm low MBH : 44 +/- 19 days <lag>3mm high MBH: 1 +/- 20 days
<lag>28mm low MBH : 118 +/- 31 days <lag>28mm high MBH: 46 +/- 13 days
different behavior ?
DCCF analysis!First results
<lag>cm: up to 150 days <lag>short mm: drop to ~ 0-20 days
delay origin: synchrotron self-absorption/opacity (e.g. Pushkarev et al. 2010)
1) pos. delay: gamma from inside “mm-core”
2) distance between “gamma-origin” and radio τ=1 surface (VLBI jet speeds, var. Doppler factors, viewing angles): Δr ~ 0 - 0.4 pc (3, 2 mm), ~ 8 pc (cm)
Fuhrmann et al. in prep.
APEX sub-mm vs. Fermi/LAT (see poster by Larsson et al.)
mm/sub-mm and gamma-ray emission regions co-spatial (within the given uncertainties)
SED modeling:
including the mm/sub-mm bands should be considered!
DCCF analysis First results
PRELIMINARY APEX 0.8 mm (38 sources)
<lag>sub-mm: 7 +/- 7 days <lag>sub-mm BL Lacs: -12 +/- 12 days <lag>sub-mm FSRQs: 13 +/- 9 days
Larsson et al. in prep.
Radio variability!Is the overall flaring behavior in agreement with shocks on pc-scales?
Shock-in-jet model - each variability model: characteristic signatures in the time and spectral domain
- e.g. shock scenario (Marscher & Gear 1985, Türler et al. 2000)
- seen as standing/moving VLBI components/features in the core region and downstream on pc-scales
Courtesy of M. Türler Courtesy: MOJAVE program
semi-analytical model calculations:
0 50 100 150 200frequency [GHz]
-300
-200
-100
0
time
lag
(wrt.
2.6
GH
z) [d
ays]
whole sampleaveraged delays
1 10 100 1000Rest Freq. [GHz]
-2.5
-2
-1.5
-1
-0.5
0
0.5
1
1.5
log(
Std.
Dev
.)
[Black]:All sources, [Red]: FSRQ, [Green]: BL Lacs
flare amplitude vs. freq. flare time delay vs. freq.
- standard shock model (Marscher & Gear 1985)
- Fromm et al. (2011): calculations for (a typical) blazar (CTA 102)
- a conical jet (p = 1)
- a toroidal magnetic field (b = 1.2)
- a constant Doppler factor
- predictions for variability amplitude and time delays
Radio variability!Is the overall flaring behavior in agreement with shocks on pc-scales?
1 10 100 1000Rest Freq. [GHz]
-2.5
-2
-1.5
-1
-0.5
0
0.5
1
1.5
log
(Std
. Dev
.)
sample average
Variability amplitude vs. frequency
Time domain - F-GAMMA radio vs. model:
a) Variability amplitude: 0 50 100 150 200
frequency [GHz]
-300
-200
-100
0
time
lag
(wrt.
2.6
GH
z) [d
ays]
whole sampleaveraged delays
1 10 100 1000Rest Freq. [GHz]
-2.5
-2
-1.5
-1
-0.5
0
0.5
1
1.5
log(
Std.
Dev
.)
[Black]:All sources, [Red]: FSRQ, [Green]: BL Lacs
flare amplitude vs. freq.
- quantity: light curve standard deviations: “intrinsic values” using a likelihood method (Richards et al. 2011)
- sample averages: clear overall increase, max: ~ 60-80 GHz, then plateau/decreasing trend?
- individual source patterns: a) increase up to mm bands b) peak and subsequent decrease c) “flat behavior” - a) + b): good agreement with growth/plateau/decay phase of shocks, c) different mechanism? - F-GAMMA covers all stages of shock evolution!
- individual source studies/modeling (single flares, max., slopes): constrain model parameters (B-Field, non-conical geometry, shock-shock interaction etc.)
- growth: APEX band important ! optical bands?
Radio variability!Is the overall flaring behavior in agreement with shocks on pc-scales?
variability amplitude vs. freq.
- detailed Discrete Cross-Correlation Function analysis (DCCF) between 2.6 and 140 GHz (110 – 2 mm)
- ~ no lags at high frequencies
- increasing lags towards lower frequencies
- overall good agreement with model predictions
0 50 100 150 200frequency [GHz]
-300
-200
-100
0
time
lag
(wrt.
2.6
GH
z) [d
ays]
whole sampleaveraged delays
1 10 100 1000Rest Freq. [GHz]
-2.5
-2
-1.5
-1
-0.5
0
0.5
1
1.5
log(
Std.
Dev
.)
[Black]:All sources, [Red]: FSRQ, [Green]: BL Lacs
flare time delay vs. freq.
0 50 100 150 200frequency [GHz]
-300
-200
-100
0
time
lag
(wrt.
2.6
GH
z) [d
ays]
whole sampleaveraged delays
1 10 100 1000Rest Freq. [GHz]
-2.5
-2
-1.5
-1
-0.5
0
0.5
1
1.5
log(
Std.
Dev
.)
[Black]:All sources, [Red]: FSRQ, [Green]: BL Lacs
time delay vs. freq.
Time domain - F-GAMMA radio vs. model:
b) sample averaged time delays:
most of the radio variability/flares produced in shocks on pc scales !
together with previous (DCCF) findings: gamma-rays likely produced in shocks on pc scales !
Radio variability!Is the overall flaring behavior in agreement with shocks on pc-scales?
Conclusions
- Fermi-LAT & F-GAMMA synergy: - timing analysis of flares/events - constraining the location of the gamma-ray emitting region
- DCCF and stacking analysis using 3.5 yrs Fermi LCs:
- first significant radio/gamma-ray correlations - strongly decreasing lags towards mm/sub-mm bands (lags 0)
- ~ 0-0.4 pc: emitting regions co-spatial!
- possible differences for FSRQs/BL Lacs and for physical parameters like BH mass
- radio variability in overall good agreement with shocks on pc-scales
gamma-rays likely produced in shocks on pc-scales!