investigation of carbonaceous interstellar dust...
TRANSCRIPT
Belén Maté,Miguel Jiménez-Redondo, Isabel Tanarro, Miguel Moreno, and
Victor HerreroInstituto de Estructura de la Materia (IEM-CSIC), Serrano 123, 28006,
Madrid, Spain
ISMS - 70TH MEETING - JUNE 22-26, 2015 - CHAMPAIGN-URBANA, ILLINOIS
Investigation of carbonaceous interstellar dust analogues by infrared spectroscopy:
Effects of energetic processing
Funding: CDS2009-00038, FIS20012 -38175, FIS2013-48087-C2-1-P, ERC-2013-Syg 610256
INSTITUTO DE ESTRUCTURA DE LA MATERIA
INSTITUTO DE ESTRUCTURA DE LA MATERIA
Interstellar hydrocarbon dust
IR absorptionfeatures
3.4 m bandJ. Chiar et al. ApJ 2013, 770, 78A. P. Jones ASP Conf. Ser. 414, 2009
Carbonaceous dust in the diffuse ISM
E. Dartois et al. A&A, 2007, 463, 635
Hydrogenated amorphous carbon (HAC or a-C:H) produced in the laboratory
CH aromatic
(upper limit)
CCaromatic
+ olefinic
CH Aliphaticstretchings
CHaliphaticbendings
Structure estimates by Dartois et al. suggest an important contribution of
hydrogen rich aliphatic carbon
Aliphatic features are more prominent
their absorption strengths are much higher
Carbonaceous dust in the diffuse ISM
J. Chiar et al. ApJ , 2013, 770, 78
Left: weighted average of the spectra of the six quintuplet lines of sight. Right: ISO spectra
UKIRT spectra toward the Galactic center Quintuplet Cluster
Structure estimates by Chiar et al.suggest that the dust is hydrogen poor
and highly aromatic
HAC film deposition in CH4/He plasmaIEM-CSIC
• CH4(40%)/He 0.3 mbar
• 40 W , 13.56 MHz
outside the coilHAC1
inside the coilHAC2
Inductively coupled RF discharge reactor
Film thickness ~ 3 µm
1 hour
IR spectra of the deposits
3000 2500 2000 1500 1000
0,0
0,1
0,2
0,3
0,4
0,5
ab
sorb
ance
wavenumber / cm-1
CH stretch C=Cstretch
CHx bend
AromaticsAliphatics
Outside the coil
Inside the coil x5
6.9 µm6.2 µm
11.3 µm
CH3 CH3CH2
7.2 µmCH3
CH2
CH3
3.4 µm
B. Maté et al. Faraday Disc. 2014, 168, 267
HAC 1
HAC 2
Analysis of HAC spectra
H 0.33
sp2 0.55
sp3 0.11
3200 3000 2800 1800 1700 1600 1500 1400 1300
0,00
0,05
0,10
0,15
0,20
0,25
Math X1
0,0
0,1
0,2
0,3
0,4
Abs
orba
nce
3200 3800 2800 1700 1500 1300Wavelength/ cm-1
0.4
0.2
0.2
0.1
Abso
rban
ceCH2, CH3sp3
CCsp2
CHsp2
HAC 1
HAC 2H 0.13
sp2 0.83
sp3 0.04
Using absorption strengths from Chiar et al. ApJ 2013, 770, 78
CO?
HAC2HAC1
3,2 3,3 3,4 3,5 3,6
-0,20
-0,15
-0,10
-0,05
0,00
5,5 6,0 6,5 7,0 7,5
3,2 3,3 3,4 3,5 3,6
-0,8
-0,4
0,0
5,6 5,8 6,0 6,2 6,4 6,6
Comparison with observations in the diffuse ISM
Infrared Galaxy IRAS 08572+3915Dartois et al. A&A 2007
Galactic center Quintuplet Cluster.Chiar et al. ApJ, 2013,
Opt
ical
dep
th
Wavelength µm
3,2 3,3 3,4 3,5 3,6
-0,20
-0,15
-0,10
-0,05
0,00
5,5 6,0 6,5 7,0 7,5
3,2 3,3 3,4 3,5 3,6
-0,8
-0,4
0,0
5,6 5,8 6,0 6,2 6,4 6,6
Comparison with observations in the diffuse ISM
Infrared Galaxy IRAS 08572+3915Dartois et al. A&A 2007
Galactic center Quintuplet Cluster.Chiar et al. ApJ, 2013,
Opt
ical
dep
th
Wavelength µm
HAC 1 spectrum scaled to the maximum
3,2 3,3 3,4 3,5 3,6
-0,20
-0,15
-0,10
-0,05
0,00
5,5 6,0 6,5 7,0 7,5
3,2 3,3 3,4 3,5 3,6
-0,8
-0,4
0,0
5,6 5,8 6,0 6,2 6,4 6,6
Comparison with observations in the diffuse ISM
Infrared Galaxy IRAS 08572+3915Dartois et al. A&A 2007
Galactic center Quintuplet Cluster.Chiar et al. ApJ, 2013,
Opt
ical
dep
th
Wavelength µm
HAC 1 spectrum scaled to the maximum
HAC 2 spectrum scaled to the maximum
3000 2000 1000
0.00
0.01
0.02
0.03
abso
rban
ce
wavenumber cm-1
Deposit growth and structure
3000 2900 2800
0.00
0.01
0.02
0.03
abso
rban
ce
wavenumber cm-1
The H/C and sp3/sp2 ratios decrease with growing thickness
Inside the coil
3 min ~ 100 nm6 min ~ 200 nm12 min ~ 400 nm
H2 plasma 0.25 mbar, 40 W
0 min 4 min
10 min
Processing in H2 plasma
The CC stretch band remainsunchanged
CC bonds polyaromatic ratherthan olefinic
The CHx stretch band decreases with
processing
CC
Summary and conclusions
• Carbonaceous dust analogues have been grown in inductively coupled RF discharges of He+CH4.
• The position in the plasma reactor affects the structure of the deposited hydrocarbon. Inside coil deposits are good
analogues to interstellar medium dust.
• Processing with H2 plasma do not affect the aromatic component of the carbonaceous material.
Belén Maté, [email protected] DE ESTRUCTURA DE LA MATERIA
INSTITUTO DE ESTRUCTURA DE LA MATERIA