Integral field spectroscopy of the Red Rectangle: Unraveling the carrier of the RRBs in 2D. Damian...
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![Page 1: Integral field spectroscopy of the Red Rectangle: Unraveling the carrier of the RRBs in 2D. Damian Kokkin, Robert Sharp, Masakazu Nakajima, and Timothy.](https://reader036.fdocuments.in/reader036/viewer/2022062314/56649f085503460f94c1d58e/html5/thumbnails/1.jpg)
Integral field spectroscopy of the Red Rectangle: Unraveling the carrier of the RRBs
in 2D.
Damian Kokkin, Robert Sharp, Masakazu Nakajima, and Timothy
Schmidt
![Page 2: Integral field spectroscopy of the Red Rectangle: Unraveling the carrier of the RRBs in 2D. Damian Kokkin, Robert Sharp, Masakazu Nakajima, and Timothy.](https://reader036.fdocuments.in/reader036/viewer/2022062314/56649f085503460f94c1d58e/html5/thumbnails/2.jpg)
The Red Rectangle
Central binary: 1915
Nebula: 1973
Distance: 330-710pc
Expelling carbon rich material
Rich optical spectrum
Cohen M., Winckel, H.V., Bond, W.E., Gull, T.R., AJ, 2004, 127, 2362
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The Red Rectangle Bands
• Emission features close to DIB wavelengths
• Exhibit a steep blue edge with a red degraded tail
Sarre, Science 269, 1995
Are the DIBs and RRBs from the same carrier molecule?
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Hi-res IFU spectra of Red Rectangle
2 nights observing at Very Large Telescope (Chile)28th-30th December 2004
5 telescope pointings
Integral field unit givesA spectrum per pixel
-Can chemically map the nebula!
![Page 5: Integral field spectroscopy of the Red Rectangle: Unraveling the carrier of the RRBs in 2D. Damian Kokkin, Robert Sharp, Masakazu Nakajima, and Timothy.](https://reader036.fdocuments.in/reader036/viewer/2022062314/56649f085503460f94c1d58e/html5/thumbnails/5.jpg)
The Red Rectangle bands and C2
T. W. Schmidt, D. L. Kokkin, S. H. Kable, R. G.
Sharp and R. Glinski (2006)
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v=0
v=1
v=2
v=0
v=1
v=2
a3Pu
d3Pg
516nm 563nm
Swan bands first observed in 1802!
Described in 1857 by W. Swan
What we are actually seeing
![Page 7: Integral field spectroscopy of the Red Rectangle: Unraveling the carrier of the RRBs in 2D. Damian Kokkin, Robert Sharp, Masakazu Nakajima, and Timothy.](https://reader036.fdocuments.in/reader036/viewer/2022062314/56649f085503460f94c1d58e/html5/thumbnails/7.jpg)
C2 is seen in comets and other things
![Page 8: Integral field spectroscopy of the Red Rectangle: Unraveling the carrier of the RRBs in 2D. Damian Kokkin, Robert Sharp, Masakazu Nakajima, and Timothy.](https://reader036.fdocuments.in/reader036/viewer/2022062314/56649f085503460f94c1d58e/html5/thumbnails/8.jpg)
Extending C2 Observations on RR
• 27th and 28th December 2006
• Target band systems:– Swan origin and Δv =
+1
– Phillips (2,0)
– c-d origin
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Observational Methodology
N
E
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Observational Methodology
Band Night Arm Grating Range (Å) Resolution (Å) ExposureSwan 27th December Blue 2500V 5091-5458 0.366-0.411 10x30 min(0,0) 2006 5hrs
Swan 28th December Blue 2500V 4598-4993 0.391-0.43 10x30 min(1,0) 2006 5hrs
c-d 28th December Red 1000I 8541-9630 1.112-1.191 10x30 min(0,0) 2006 5hrs
Phillips 28th December Red 1000I 8541-9630 1.112-1.191 10x30 min(2,0) 2006 5hrs
RRBs 27th December
2006
Red 2000R 5620-6124 0.492-0.538 6x30min3hrs
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Further Swan bands of C2 in the RR
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C2 versus stellar emission
C2 Swan
origin
emission
Stellar
emission
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Distance from object versus emission
1 5
10
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More on the RRBs
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RRBs with distance
1 5
10
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Maps from the red arm
ERE
Emission
5800Å RRB
emission
Sodium
doublet
emission
5850Å RRB
emission
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The ModelModeling: C2 Swan Origin
Assumes C2 is statistical equilibrium with the stellar radiation field.
Includes the 6 lowest electronic states and for each of these 0≤υ≤5 and 0≤J≤100 giving 8484
distinct ro-vibronic states for transtions to occur between.
Photophysics simulated by a Monte Carlo Markov chain starting in a random state.
Modeling: λ5800Å RRB and the C2 Swan Origin
The observed fluorescence on Earth
NW
F FTOTAL 23
7
)1026.206(4
10
237 )1026.206(410
TOTAL
FF
BN
10
2
230
7
1015.3
)1026.206(1610
e
mFfN TOTAL
F
At
5arcsec
If the oscillator strength of the λ5800Å RRB is 0.01 which is common for most medium to large PAH systems
and unity fluorescence yield then the abundance would be larger then C2. This approach the C2 column density
when f approaches unity.
Rate of any transition
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Electronic Energy Levels
v=0
v=1
v=2
v=0
v=1
v=2
a3
Π u
d3
Πg
v=0
v=1
v=2
X1
Σg+
v=0
v=1
v=2
A1
Πu
Swan systemPhillips system
v=0
v=1
v=2
b3
Σg-
Ballik-Ramsay system
v=0
v=1
v=2
c3
Σu+
c-d system
X-a forbidden transitions
X-c forbidden transitions
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Computational Methods
core
Valence active space
external
MOLPRO package
CASSCF reference states generated
aug-cc-pVxZ (x = D, T, Q, 5, 6)
Swan system used to validate calculations, then applied aV6Z to other systems:
Phillips, Ballik-Ramsay, c-d
MRCI: excitations into external space
Transition moments calculated by MOLPRO
Vibrational wavefunctions obtained from ab initio PESs to calculated state-
to-state f-values, Einstein coefficients & radiative lifetimes
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Swan System - PES
D T Q 5 6
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Swan System – Other Properties
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c-d system
Radiative Lifetime: 4.72μsOscillator Strength:
0.0054
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Direct observation of c-d system
• 1% premix of C2H2 in Ar
• DC Discharge
• Detection via LIF
v=0
v=1
v=2
v=0
v=1
v=2
a3Pu
d3Pg
v=0
v=1
v=2
v=3
c3
Σu+
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High resolution
Kokkin, Reilly, Morris, Nakajima, Nauta, Kable, Schmidt, JCP, 125, 231101 (2006)
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Conclusions
• Further C2 swan emission lines were detected
in the Red Rectangle.– C2 Swan origin and Δv = +1
– No detection of Phillips (2,0) and c-d origin
• Opens modelling opportunities of C2 in Red Rectangle.
• Characterise local environment• Physical properties of RRBs carrier
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Acknowledgements
• Neil Reilly, Scott Kable, Klaas Nauta
• George Bacskay