Bar-driven Spirals?
S4G perspective
Heikki Salo, Univ. Oulu, Finland
Dynamics of Disk Galaxies workshop, Seoul 21.10.2013 Thanks to: Eija Laurikainen, Simon Diaz, Martin Herrera, Jarkko Laine, Sebastien Comeron + S4G team
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Bar-driven Spirals? S 4 G perspective Heikki Salo, Univ. Oulu, - - PowerPoint PPT Presentation
Bar-driven Spirals? S 4 G perspective Heikki Salo, Univ. Oulu, Finland Dynamics of Disk Galaxies workshop, Seoul 21.10.2013 Thanks to: Eija Laurikainen, Simon Diaz, Martin Herrera, Jarkko Laine, Sebastien Comeron + S 4 G team 1 TOPIC: What is
Heikki Salo, Univ. Oulu, Finland
Dynamics of Disk Galaxies workshop, Seoul 21.10.2013 Thanks to: Eija Laurikainen, Simon Diaz, Martin Herrera, Jarkko Laine, Sebastien Comeron + S4G team
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(Spitzer Survey of Stellar Structure in Galaxies, PI K. Sheth)
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Different scenarios (see Jerry Sellwood’s review on Tuesday) 1) Spiral = direct extension of bar mode
Either in the sense of classical density wave picture or in manifold-theory (Lia Athanassoula on Tuesday)
2) Spiral mode is coupled to bar via resonance coupling 3) Spiral is an independent mode or transient pattern, not connected to the bar Not easy to distinguish these scenarious based on morphology: 1) ⇒ Expect correlation between amplitude of bars and spirals Same pattern speed ⇒ phases also related 2) ⇒ Correlation between amplitudes 3) ⇒ No correlation
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OSUBGS Buta et al. 2005
0.0 0.2 0.4 0.6 0.8 maximum FT/FR (BAR) 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 maximum FT/FR (SPIRAL)
GD-spirals more frequent in barred (Kormendy 1979, D & B Elmegreen 1982)
bar-related torque strength Qb strongly correlated with spiral-related Qs
possible weak correlation between Qb and Qs
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50 100
50 100
NGC 1452 2.2µm
20 40 60 80 100 r (arcsec) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2
bar
max A2
20 40 60 80 100 r (arcsec) 0.0 0.2 0.4 0.6 0.8 FT/FR
/home/heikki/NGC1566_OULU2011.dir/NGC1452_schema_beijing2012 heikki@pc091079 Sun Oct 20 08:42:57 2013
Azimuthal Fourier amplitudes of density
(e.g. Elmegreen & Elmegreen 1985)
I(r, φ) = I0(r) " 1 +
m=∞
X
m=1
Am(r) cos [m (φ − φm(r))] #
Tangential force amplitudes (normalized to axisymmetric force) (Combes and Sanders 1981)
F T/F R = max(|FT (r, φ)|) < |FR(r, φ)| > (≡ F T/F R in this talk)
⇒ maximum at bar region = Qb
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100 200
100
ngc1566
50 100 150 200 0.0 0.5 1.0 A2 Rbar R2s
bar spirals
50 100 150 200 r (arcsec) 0.0 0.1 0.2 0.3 FT/FR
bar spirals bar+spiral
Separate non-axisymmetric bar and spiral contributions to density ⇒ A2(bar), A2(spiral) Qb, Qs
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NGC936 NIRSOS 2MASS 2MASS: uncleaned
20 40 60 80 100 rad (") 0.0 0.1 0.2 0.3 FT/FR
CART POLAR: mMAX =8 mMAX =6 mMAX =4 mMAX =2
20 40 60 80 100 rad (") 0.0 0.1 0.2 0.3 20 40 60 80 100 rad (") 0.0 0.1 0.2 0.3
(Salo et al. 1999, AJ 117, 792; Laurikainen and Salo 2002 MNRAS 337, 1118) (Applied to to 2MASS, OSUBSGS, NIRSOS, AAT samples in Buta et al. and Laurikainen et al. studies)
(M/L= constant, or a function of radius)
vertical scale height hz
(e.g. from hr or RK20; several choices for vertical profile exp, sech2, gaussian ...) 2-fold uncertainty in hz ⇒ <25% uncertainty in Qb
+ polar FFT force integration directly from m-components) azimuthal filtering
⇒ no spurious force peaks in the noisy outer disk
= Important advantage
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0.0 0.5 1.0 1.5 max A2 (spiral) 0.0 0.2 0.4 0.6 0.8 1.0 max Qbar a) 0.0 0.5 1.0 1.5 max A2 (spiral) 0.0 0.1 0.2 0.3 0.4 0.5 Qbar (R=R2s) b)
R2s/Rbar<1.5 R2s/Rbar>1.5 R2s/Rbar<1.5 R2s/Rbar>1.5
Salo, Laurikainen, Buta, Knapen 2010:
⇒ explain earlier inconclusive resuts
spiral amplitude A2(r) against the gravity forcing by bar at the same distance, Qbar(r) (instead of using the maximum values) Example: Buta et al. (2009) deep AAT-sample: No correlation: max of Qbar and max of A2(spiral) Clear correlation: between local forcing due to bar, if evaluated at the location of radial maximum of spiral A2
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0.0 0.1 0.2 0.3 Qbar(r) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2(r)
r/Rbar= 1.1
rsample = 0.64 p = 1.3e-11 0.00 0.05 0.10 0.15 Qbar(r) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2(r)
r/Rbar= 1.3
rsample = 0.57 p = 1.2e-08 0.00 0.02 0.04 0.06 0.08 Qbar(r) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2(r)
r/Rbar= 1.5
rsample = 0.30 p = 0.0040 0.00 0.01 0.02 0.03 0.04 Qbar(r) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2(r)
r/Rbar= 1.7
rsample = 0.074 p = 0.26
For both OSUBSGS and AAT -samples:
Statistically significant correlation between local bar forcing and local spiral amplitude up to 1.5 bar lengths
(Salo et al. 2010)
m > 0 density amplitude set to zero for r > Rbar in calculation of forces correlation between local FT/FT and A2 looked at 4 different distances outside the bar
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NGC1097 .SBS3.. uc=0
50 100 150 200 250 300 a (arcsec) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 ELLIP max: 95.1" 0.646 min: 120.6" 0.513 50 100 150 200 250 300 a (arcsec) 50 100 150 200 PA dPA -28.2
100 200 arcsec
100 200
BARLEN = 96.2" (sky-plane) uc=0
Need: Sky-subtracted, cleaned images Reliable (=visually checked) galaxy orientation parameters (P4) and bar lengths Calculation of Fourier amplitudes and forces
Original S4G with 2352 galaxies ⇒ bar force calculated for 532 galaxies
removed 374 ’bad’ cases (too small FOV, image defects, bright star, large sky-gradient, superposed companion, deformed, or with unreliable orientation) ⇒ 1978 galaxies limit to i < 65◦ ⇒ 1172 galaxies barred (bar length can be estimated) ⇒ 786 galaxies barred + trailing/leading sense of spirals visible ⇒ 729 galaxies force calculations so far for 532 galaxies
Example of bar length measurements: visual bar length, position angle, max ellipticity (Martin Herrera / Simon Diaz)
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ALL SB, SAB
0.0 0.2 0.4 0.6 0.8 1.0 Qb (bar) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2(spir) N_SB =261 0.269 p=0.0000 N_SAB=227 0.286 p=0.0000
For S4G-sample: (Salo et al. in preparation) Significant correlation between max Qb(bar) and max A2(spiral) Holds both for strongly (SB) and weakly-barred (SAB) galaxies
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ALL SB, SAB
0.0 0.2 0.4 0.6 0.8 1.0 Qb (bar) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2(spir) [1.5 < R/Rbar < 2.0] N_SB =282 0.314 p=0.0000 N_SAB=238 0.345 p=0.0000
ALL SB, SAB
0.0 0.2 0.4 0.6 0.8 1.0 Qb (bar) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2(spir) [2.5 < R/Rbar < 3.0] N_SB =279 0.199 p=0.0008 N_SAB=233 0.246 p=0.0002
ALL SB, SAB
0.0 0.2 0.4 0.6 0.8 1.0 Qb (bar) 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2(spir) [3.0 < R/Rbar < 3.5] N_SB =264 0.244 p=0.0001 N_SAB=223 0.252 p=0.0001
1.5 - 2.0 Rbar 2.5 - 3.0 Rbar 3.0 - 3.5 Rbar
max FT/FR(BAR) vs. A2(R)
1 2 3 4 R/Rbar 0.0 0.2 0.4 0.6 0.8 rank correlation
SB 236 SAB 203
The correlation of max Qbar and max spiral A2 is significant even at ≈ 3 bar radii.
rank correlation between Qbar and A2(r) as a function of R/Rbar Symbols: correlation significant (p < 0.02)
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max FT/FR(BAR) vs. A2(R)
1 2 3 4 R/Rbar 0.0 0.2 0.4 0.6 0.8 rank correlation
SB 236 SAB 203
local FT/FR(BAR) vs. A2(R)
1 2 3 4 R/Rbar 0.0 0.2 0.4 0.6 0.8 rank correlation
SB SAB
GLOBAL LOCAL Correlation between local Qbar and local spiral A2 even stronger near the bar, but drops more rapidly with distance
(consistent with salo et al. 2010: local values showed correlation, global not)
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T-interval = -3,-1
0.0 0.2 0.4 0.6 0.8 1.0 Qb 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2_spir
N_SB= 19 0.498 N_SAB= 15 0.757*
T-interval = -1, 1
0.0 0.2 0.4 0.6 0.8 1.0 Qb 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2_spir
N_SB= 42 0.188 N_SAB= 46 0.329
T-interval = 1, 3.5
0.0 0.2 0.4 0.6 0.8 1.0 Qb 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2_spir
N_SB= 37 0.404* N_SAB= 48 0.390*
T-interval = 3.5, 6
0.0 0.2 0.4 0.6 0.8 1.0 Qb 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2_spir
N_SB= 22 0.654* N_SAB= 55 0.405*
T-interval = 6, 8
0.0 0.2 0.4 0.6 0.8 1.0 Qb 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2_spir
N_SB= 76 0.401* N_SAB= 31 0.263
T-interval = 8, 10
0.0 0.2 0.4 0.6 0.8 1.0 Qb 0.0 0.2 0.4 0.6 0.8 1.0 1.2 A2_spir
N_SB= 90 0.372* N_SAB= 44 0.489*
S4G sample size (at least almost) large enough to allow further division to subsamples:
max Qbar and local spiral A2 for different types:
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200 400
200 400
NGC1097
200 400
200 400
PA= 126.5 INC= 48.1
200 400
200 400
SB (R’) 3.30000
100 200 300 400 100 200 300 400
resized z
Above: spiral amplitude correlates with bar amplitude up to 3 bar radii
How are bar and spiral phases connected?
Address by using stacked S4G images
⇒ ’S’)
bar radius = 50 units (red circle) image region 500 × 500 untis masks scaled in similar fashion 15
1 2 3
1 2 3
T-interval = 1, 3.5
1 2 3
1 2 3
unsharp mask
/home/heikki/P4_JUTTU_PRO/KOREA_STACK/s4g_stack_2013_korea_ttypes_example heikki@pc091079 Sat Oct 19 15:38:46 2013
EXAMPLE: Stacked aligned/scaled image for all SB galaxies with 1 < T <3.5
Inner ring/ ansae visible in stacked image no trace od spirals?
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1 2 3
1 2 3
T-interval = 1, 3.5
1 2 3
1 2 3
subtract folded image
/home/heikki/P4_JUTTU_PRO/KOREA_STACK/s4g_stack_2013_korea_ttypes_example2 heikki@pc091079 Sat Oct 19 15:38:46 2013
Spiral contrast is weak (≈ 0.2 mag)
Highlight by subtracting an image folded along the bar axis display only positive brightness ⇒ spiral residuals visible in the I and III quadrants (’S’) between 1-2.5 Bar radii
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1 2 3
1 2 3
T-interval = 1, 3.5
1 2 3
1 2 3
subtract folded image
/home/heikki/P4_JUTTU_PRO/KOREA_STACK/s4g_stack_2013_korea_ttypes_example2_random heikki@pc091079 Sat Oct 19 15:38:47 2013
How does one know that the residual is not due to single prominant spiral? Randomize position angles of bars before stacking:
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T-interval = -3,-1
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = -1, 1
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = 1, 3.5
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = 3.5, 6
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = 6, 8
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = 8, 10
/home/heikki/P4_JUTTU_PRO/KOREA_STACK/s4g_stack_2013_korea_ttypes_dens heikki@pc091079 Thu Oct 17 19:42:36 2013
Apply similar analysis to SB’s of different morphological types Average surface-brightness images
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T-interval = -3,-1
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = -1, 1
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = 1, 3.5
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = 3.5, 6
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = 6, 8
20 40 60 80 100 120 140 20 40 60 80 100 120 140T-interval = 8, 10
/home/heikki/P4_JUTTU_PRO/KOREA_STACK/s4g_stack_2013_korea_ttypes_dens2 heikki@pc091079 Thu Oct 17 19:42:37 2013
Folded spiral residuals: Seem to indicate coherent spiral phases wrt to bar
(excluding the earliest bin) 20
1 2 3 R/Rbar 0.0 0.1 0.2 0.3 0.4 0.5 0.6 A2 density
1 - 3.5 3.5 - 6 6 - 8 8 -10 1 2 3 R/Rbar 0.0 0.2 0.4 0.6 FT/FR 1 2 3 R/Rbar
0.0 0.2 φ2 density 1 2 3 R/Rbar
0.0 0.2 φ2 potential
/home/heikki/P4_JUTTU_PRO/KOREA_STACK/s4g_stack_2013_korea_ttypes_synte heikki@pc091079 Sat Oct 19 15:38:48 2013
More uses of synthetic Average-bar images Treat as real image ⇒ Fourier amplitudes, force profiles
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1 2 3 R/Rbar 0.0 0.5 1.0 1.5 Vrot
1 - 3.5 3.5 - 6 6 - 8 8 -10
/home/heikki/P4_JUTTU_PRO/KOREA_STACK/s4g_stack_2013_korea_ttypes_synte_vrot heikki@pc091079 Sat Oct 19 15:38:49 2013
⇒ Synthetic disk-rotation curves
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Synthetic images can be improved by stacking Fourier-smoothed images with NIRQB
From Diaz et al. (in preparation): Upper row: average density + spiral residual in folding Upper row: FT/FR forces + spiral potential residual in folding
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a large range of luminosities and bulge/total ratios. ⇒ bar/spiral connection can be addressed for a sample of ∼500 galaxies Results: 1) Statistically significant correlation between bar tangential forcing
(either max of Qb, or local FT/FR) and spiral amplitude (A2), up to about 3 bar radii
Holds both for strong (SB) and weak (SAB) bars 2) Stacked images suggest that spiral phases correlate with the bar, at least to 2 bar radi Found phase correlation strengthens the case for bar-driven spiral structure
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Future studies/studies in progress
measurements of phase and pitch angles (Martin Herrera)
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