Issue |
A&A
Volume 511, February 2010
|
|
---|---|---|
Article Number | L3 | |
Number of page(s) | 4 | |
Section | Letters | |
DOI | https://doi.org/10.1051/0004-6361/201014019 | |
Published online | 26 February 2010 |
LETTER TO THE EDITOR
A coincidence between a hydrocarbon plasma
absorption spectrum and the
5450 DIB
H. Linnartz1 - N. Wehres1,2 - H. Van Winckel3 - G. A. H. Walker4 - D. A. Bohlender5 - A. G. G. M. Tielens6 - T. Motylewski7 - J. P. Maier7
1 - Raymond and Beverly Sackler Laboratory for Astrophysics,
Leiden Observatory, Leiden University, PO Box 9513, 2300 RA
Leiden, The Netherlands
2 -
Kapteyn Astronomical Institute, University of Groningen, PO Box 800, 9700 AV Groningen, The Netherlands
3 -
Instituut voor Sterrenkunde, K.U. Leuven, Celestijnenlaan 200B, 3000 Leuven, Belgium
4 -
Physics and Astronomy Department, University of British Columbia, Vancouver, BC V6T 1Z4, Canada
5
- National Research Council of Canada, Herzberg Institute of
Astrophysics, 5071 W. Saanich Road, Victoria, BC V9E 2E7,
Canada
6 -
Leiden Observatory, Leiden University, PO Box 9513, 2300 RA Leiden, The Netherlands
7 -
Department of Chemistry, University of Basel, Klingelbergstrasse 80, 4056 Basel, Switzerland
Received 8 January 2010 / Accepted 4 February 2010
Abstract
Aims. The aim of this work is to link the broad 5450 diffuse interstellar band (DIB) to a laboratory spectrum recorded through expanding acetylene plasma.
Methods. Cavity ring-down direct absorption spectra and
astronomical observations of HD 183143 with the HERMES spectrograph on
the Mercator Telescope on La Palma and the McKellar spectrograph
on the DAO 1.2 m Telescope are compared.
Results. In the 543-547 nm region a broad band is measured with a band maximum at 545 nm and FWHM of 1.03(0.1) nm coinciding with a well-known diffuse interstellar band at 5450 with an FWHM of 0.953 nm.
Conclusions. A coincidence is found between the laboratory and
the two independent observational studies obtained at higher spectral
resolution. This result is important, as a match between a laboratory
spectrum and a - potentially lifetime broadened - DIB is found. A
series of additional experiments were performed in order to
unambiguously identify the laboratory carrier of this band, but this
was not successful. The laboratory results, however, restrict the
carrier to a molecular transient, consisting of carbon and hydrogen.
Key words: astrochemistry - techniques: spectroscopic - ISM: molecules - ISM: lines and bands
1 Introduction
Diffuse interstellar bands are absorption features observed in starlight that is crossing diffuse interstellar clouds. Since this discovery in the beginning of the 20th century, scientists have been puzzled by the origin of these bands that appear both as relatively narrow and rather broad bands covering the UV/VIS and NIR (Tielens & Snow 1995). In the last decennia, the idea has been established that it is unlikely that all these bands originate from one or a very few carriers, and with the progress of optical laboratory techniques, several families of potential carriers have been investigated. It was shown that the electronic transitions of a series of PAH-cations do not match the listed DIBs (Ruiterkamp et al. 2002; Salama et al. 1996; Bréchignac & Pino 1999; Salama et al. 1999). Similarly, systematic laboratory studies of electronic spectra of carbon chain radicals have not resulted in positive identifications either (Motylewski et al. 2000; Ball et al. 2000a; Jochnowitz & Maier 2008), even though it is known from combined radio-astronomical and Fourier transform microwave (FTMW) studies that many of such species are present in dense clouds (Thaddeus & McCarthy 2001). Only C3 has been recorded unambiguously in diffuse interstellar clouds (Maier et al. 2001).
Other studies, focusing on multi-photon excitation in molecular hydrogen (Sorokin et al. 1998), or spectra of fullerenes and nano-tubes (Foing & Ehrenfreund 1994; Kroto & Jura 1992) have been unsuccessful as well. In the past years, several coincidences between laboratory and astronomical DIB studies have been reported in the literature. These have all turned out to be accidental, and from a statistical point of view, the chance of an overlap is also quite substantial, because DIBs cover a major part of the wavelength region between roughly 350 and 1000 nm. However, there are several conditions that have to be fulfilled before any coincidence of a laboratory and an astronomical DIB spectrum may be interpreted as a real match. These conditions have become stricter with the recent improvement in achievable spectral resolution, both in laboratory and astronomical studies.
The two most important DIB matching criteria to link laboratory and astronomical data follow:
- 1.
- The gas-phase laboratory and observational values of both peak position and bandwidth of the origin band transition should be identical, unless it can be argued that a spectral shift or band profile change may come from an isotope or temperature effect. An example of the latter is given by spectroscopic measurements on benzene plasma yielding an absorption feature coinciding with the strongest DIB at 442.9 nm (Ball et al. 2000b; Araki et al. 2004). The laboratory FWHM turned out to be narrower than in the astronomical spectrum. It was argued that the spectrum of a non-polar molecule cooled in a molecular expansion may be considerably colder than in space, where only radiative cooling applies. A similar discussion has been given by (Motylewski et al. 2000), who show that unresolved rotational profiles may change substantially for different temperatures, as has also been calculated and discussed by Cossart-Magos & Leach (1990).
- 2.
- Once the origin band overlaps with a DIB feature, gas-phase transitions to vibrationally excited levels in the electronically excited state of the same carrier molecule should match as well, and the resulting band profiles should behave in a similar way (i.e. with comparable equivalent width ratios) (Motylewski et al. 2000). A good example for this is the electronic spectrum of C7- that has been regarded for several years as a potential carrier, because subsequent electronic bands fulfilled both conditions (Tulej et al. 1998; Kirkwood et al. 1998). Detailed follow-up studies show that the series of (near) matches was coincidental (McCall et al. 2001).
In this letter we report a match of a laboratory spectrum with a
diffuse interstellar band that is special, because the first condition
is fulfilled for a rather broad and potentially lifetime broadened
DIB; i.e., the laboratory and astronomical spectra should be fully
identical, independent of temperature restrictions. New astronomical
observations obtained with the Mercator telescope, using
the HERMES spectrograph and the Dominion Astrophysical Observatory
(DOA) 1.2 m telescope, using the McKellar spectrograph, are
presented in order to characterize the band profile of the
5450 DIB with the best possible resolution.
Even though we have not been able to unambiguously identify
the laboratory carrier, which is most likely a smaller hydrocarbon
bearing molecular transient, we think that this overlap is important
to report, since it provides a new piece in the puzzle.
2 Laboratory experiments
The experimental set-up is described in
Linnartz et al. (1998) and Motylewski & Linnartz (1999), and has been extensively used
to study many carbon chain radicals of astrophysical interest (Jochnowitz & Maier 2008). The monochromatic output 0.1 cm-1 at 540 nm (
18 500 cm-1) of a pulsed dye laser-based cavity ring-down set-up is focused into an optical cavity
consisting of two highly reflective mirrors (
R > 0.9999). A
special, pulsed high-pressure slit-nozzle system capable of producing
intense 300
s long plasma pulses by discharging (-1 kV, 100 mA)
an expanding gas mixture of 1% acetylene (C2H2) in He
is mounted inside the cavity with its slit parallel to the optical
axis of the cavity. In the expansion, a wide variety of new species
is formed, and as the technique is not mass selective, special care
has to be taken when assigning bands to specific carriers.
Mass selective matrix isolation spectra offer a good starting point for
an assignment (Jochnowitz & Maier 2008). In the case of rotationally
resolved spectra, unambiguous identifications are generally possible,
either by combination differences of accurate spectral fits, or by
isotopic studies using C2D2 instead of C2H2 (or a mixture
of C2H2/C2D2). The source runs at 30 Hz, and special care is
taken that the pressure inside the cavity remains constant during jet
operation to reduce baseline fluctuations. Rotational temperatures
are typically
10-20 K. This low
temperature results in a spectral simplification and simultaneously
increases the detection sensitivity because of improved
state density. In addition, the source offers a Doppler free
environment with a relatively long effective absorption path length.
The laser beam intersects the 3 cm long planar expansion about
5-10 mm downstream using a sophisticated trigger scheme. Subsequent
ring-down events (typically 20-30
s for a 52 cm long cavity)
are recorded as a function of the laser frequency by a photo-diode
and transferred to an averaged ring-down time by fitting 45 subsequent ring-down events. This value as function of the
laser wavelength provides a sensitive way to record optical spectra.
An absolute frequency calibration is obtained by recording an I2reference spectrum simultaneously.
![]() |
Figure 1:
The |
Open with DEXTER |
3 Astronomical observations
The laboratory data are compared to observations from two different astronomical facilities.
3.1 HERMES @ Mercator telescope
The HERMES observations were carried out in service mode using the
Mercator telescope at Roque de los Muchachos Observatory on La Palma.
The 1.2 m telescope is operated by the Katholieke Universiteit in
Leuven, Belgium, in collaboration with the Observatory in Geneva,
Switzerland.
The spectra were obtained in June 2009 with HERMES (High Efficiency
and Resolution Mercator Echelle Spectrograph) (Raskin & Van Winckel 2008),
which is a fibre-fed-cross-dispersed spectrograph.
The spectrograph has a fixed spectral format and samples the spectrum
between 377 and 990 nm in 55 spectral orders on a 4.6 k
2 k CCD.
The spectral resolution is slightly variable over the field,
but is 85 000 on average. We obtained 3 spectra of 1200 s of
HD 183143 (B7Ia, m(v)=6.92,
B-V=+1.001), the DIB spectral standard
with a reddening E(B-V) close to 1.0. The reference star HD 164353
(
B5Ib, m(v)=3.97,
B-V = - 0.002) was sampled in 3 exposures of 1 min.
The spectral reduction was performed using the specifically coded
HERMES pipeline, and it contains all the standard steps in spectral reduction.
The wavelength calibration is based on spectra of ThAr and Ne lamps.
As we are mostly interested in the broad absorption feature that
is centred around 545 nm, we focus further on this spectral region
of HD 183143. The spectra are shown in Fig. 1 (middle rows) and
compared to the
5450 DIB profile as available from a
series of digital DIB catalogues
(Galazutdinov et al. 2000; Tuairisg et al. 2000; Jenniskens & Desert 1994; Herbig 1975)
in the upper row.
3.2 McKellar @ DAO telescope
Fifty-five half-hour spectra were taken with the McKellar Spectrograph
and SITe-4 CCD at the DAO 1.2 m telescope, operated by the National
Research Council of Canada, over 6 nights between 16 and 23 July 2006
(UT) at a dispersion of 10.1 Å/mm giving 0.151 Å/pixel
for a resolution 0.3 Å. The data were processed in a
standard fashion using IRAF
.
The aggregate spectrum had a
signal-to-noise ratio of about 1200/pixel before correction of telluric lines.
Removal of the quite weak telluric features was performed conventionally
with spectra (
)
of the A0 V star zeta Aql (HD 177724) as the template.
Rigel, an unreddened comparison star with a B8 Ia spectral type very similar to the B7 Ia of HD 183143 was also observed to identify photospheric lines that contaminate the interstellar features observed in the latter star. The sharp line at approximately 5454 Å arises from S II and was removed from the spectrum of HD 183143 by simply fitting a Voigt profile to the line and subtracting this from the original spectrum. The final ``deblended'' spectrum is plotted as a comparison in Fig. 1 (lower panel, middle spectrum).
4 Results
In Fig. 2 several spectra in the 543-547 nm region are compared.
The top spectrum is the digital DIB spectrum of the 5450
DIB (Galazutdinov et al. 2000; Tuairisg et al. 2000; Jenniskens & Desert 1994; Herbig 1975).
The spectrum in the middle is a zoom-in on the
deblended McKellar spectrum as shown in Fig. 1. The bottom spectrum
is the laboratory spectrum recorded in direct absorption through
an expanding 1% C2H2/He plasma. The similarity between
the three spectra is striking.
This wavelength region was initially scanned to search for the
1u - X1
g+ electronic origin band
spectrum of the linear carbon chain radical C7 (following the
C7- DIB discussion) that was located in matrix isolation
experiments around 542.3 nm. The laboratory spectrum, shown in
Fig. 2, consists of many narrow lines that come from small
acetylene fragments (typically C2 and CH) that get weaker
when the distance from the nozzle orifice to the optical axis is increased,
but there is clearly a broad underlying feature.
As this band shifts by 1.5 nm to the red upon C2D2 precursor
substitution, it was initially neglected, because both
C2H2 and C2D2 should result in an identical spectrum for C7.
The shift is illustrated in Fig. 3. In addition, the deuterated spectrum
appears to be somewhat stronger. Despite this
negative result for C7, the profile hiding under the narrow
lines in the C2H2 precursor experiment perfectly matches the
5450 DIB available from the DIB databases, which is one reason
additional observations were performed.
![]() |
Figure 2:
The top spectrum shows the digital |
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![]() |
Figure 3: Comparison between laboratory experiments sampling expanding plasma using regular acetylene ( top) and deuterated acetylene ( bottom) as a precursor gas. |
Open with DEXTER |
5 Discussion
There is little discussion possible about the coincidence between the
recorded laboratory spectrum and the 5450 DIB. Both bands
have a central peak position of 545 nm and an FWHM of 1.03 (0.1) nm
(laboratory spectrum) and 0.953 nm (observational spectrum)
(Tuairisg et al. 2000). The uncertainty in the first value comes from
the overlap of the many individual transitions, which prohibits a clear
view of the broad feature. The question is more whether this actually
represents a DIB match, and for this complementary information is
needed. Additional laboratory work was performed, where it
should be noted that the scans shown in Figs. 2 and 3 typically last
45 min to an hour, in order to achieve the required sensitivity
and to cover a frequency domain broad enough to differenciate band
profile and base line; i.e., fast optimizations are impossible.
The laboratory band does not show any structure that can be related
to unresolved P, Q, and R-branches. With 1.03 (0.1) nm, the band is
also much broader than the unresolved rotational profile of a larger
carbon chain radical. For comparison, at 15 K, the band profile of
the linear C6H radical (at 525 nm) is about five times narrower
(Linnartz et al. 1999). It should also be noted that such a broad
feature actually represents a large absorption compared to many of
the sharper DIBs. Changing the experimental settings to vary
the final temperature in the expansion by measuring close
(
50 K
warm
)
and far
(
10 K
cold
)
downstream does not
substantially change the FWHM of the spectral contour.
As the narrow overlapping transitions have FWHMs close to the
laser bandwidth, experimental broadening artifacts, such as residual
Doppler broadening in the expansion or amplified spontaneous emission,
can be excluded. It is clear that the band profile is caused by
a temperature-independent and carrier-specific broadening effect,
presumably lifetime broadening. The observed bandwidth of 1.0 nm
(
35 cm-1 around 545 nm) corresponds to a lifetime
of roughly 0.15 ps.
The bandwidth profile does not allow conclusions on the nature of
the laboratory carrier. The carrier must be a transient species
(a molecular radical, a cation or anion, a weakly bound
radical complex, possibly charged, or a vibrationally or
electronically excited species) because no comparable spectra are
recorded without plasma (i.e. with a regular C2H2/He
expansion). The use of a C2D2/He expansion results in
a red-shifted spectrum (Fig. 3), and from this it can be concluded
that the laboratory carrier must contain both carbon and hydrogen.
To check whether there are equivalent H-atoms in this
carrier, a C2H2/C2D2 1:1 mixture in He has been used
as an expansion gas, but this only results in a very broad
absorption feature covering the whole region where results
are found for a pure C2H2 and a pure C2D2 expansion.
It is impossible to conclude anything about the actual number of equivalent
H-atoms in the carrier by determining the number of bands that show up,
as could be demonstrated for HC6H+ or HC7H
(Khoroshev et al. 2004; Ball et al. 2000a; Sinclair et al. 1999). Also the use
of another precursor (e.g. allene) did not provide conclusive information.
Additional experiments have been performed. The 543-545 nm region
has been scanned using a two-photon REMPI-TOF experiment with the
aim determining the mass of the carrier (Pino et al. 2001). No
spectrum could be recorded, which may be related to the short
lifetime of the excited state or with the fact that the carrier
is an ion. Ions are indeed formed in this planar plasma source
(Witkowicz et al. 2004). Both smaller and larger species have
been observed, with optimum production rates depending, among
other things, on the backing pressure. The production of larger species is
generally more critical; e.g., higher backing pressures are needed,
but this also may destabilize the plasma, which is unfortunate,
particularly during long scan procedures. More complex species
are generally found further downstream, but in this specific case,
we did not observe large differences as a function of the distance
from the laser beam to the nozzle orifice. This is the typical
behaviour for a smaller constituent in the gas expansion. We tried
to systematically study the voltage dependence of the signal.
For a positive ion, an increase in voltage should go along with a
decrease in signal for distances further downstream, as the jaws
carry a negative voltage. It is the opposite for anions, but 10 years
of experience with this source have shown that negative ions are rather
hard
to produce. Again, the changes we recorded were small and did
not allow drawing hard conclusions. Following condition 2 mentioned
in the introduction, we also searched in other wavelength regions
blue-shifted by values typical for an excited C-C, C=C, CC,
or CH stretch in the upper electronic state. Such excited bands
have not been observed here, but it should be noted that these
bands can be intrinsically weak.
In summary, we are left with a laboratory spectrum that coincides both in band maximum and band width with a known DIB band at 545 nm. Our measurements show that the absorption spectrum of a transient molecule containing hydrogen and carbon reproduces the astronomical spectrum. The profile can be explained with life time broadening, and this is consistent with the observation that the laboratory and astronomical spectrum are identical; i.e., with no temperature constraints. In addition, it explains why the large bandwidth of this DIB does not vary along different lines of sight. The large effective absorption may also be indicative of an abundant carrier. The exact carrier, as such, remains an open question. The present result, however, may be useful for stimulating upcoming DIB work.
AcknowledgementsThe results presented here bridge a period of 10 years. The cavity ring-down measurements were performed in the Institute for Physical Chemistry (Department of Chemistry, University of Basel) with support of the Swiss National Science Foundation, and the analysis follows recent observations and a collaboration within the framework of the FP6 research training network The Molecular Universe. Additional financial support of NOVA is gratefully acknowledged.
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Footnotes
- ... IRAF
- IRAF is distributed by the National Optical Astronomy Observatory, which is operated by the Association of Universities for Research in Astronomy (AURA) under cooperative agreement with the National Science Foundation.
All Figures
![]() |
Figure 1:
The |
Open with DEXTER | |
In the text |
![]() |
Figure 2:
The top spectrum shows the digital |
Open with DEXTER | |
In the text |
![]() |
Figure 3: Comparison between laboratory experiments sampling expanding plasma using regular acetylene ( top) and deuterated acetylene ( bottom) as a precursor gas. |
Open with DEXTER | |
In the text |
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