Methanol maps of low-mass protostellar systems

L. E. Kristensen; E. F. van Dishoeck; T. A. van Kempen; H. M. Cuppen; C. Brinch; J. K. Jørgensen; M. R. Hogerheijde

doi:10.1051/0004-6361/201014182

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A&A, 516 (2010) A57

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Issue		A&A Volume 516, June-July 2010


Article Number		A57
Number of page(s)		16
Section		Interstellar and circumstellar matter
DOI		https://doi.org/10.1051/0004-6361/201014182
Published online		28 June 2010

A&A 516, A57 (2010)

I. The Serpens molecular core

L. E. Kristensen¹ - E. F. van Dishoeck^1,2 - T. A. van Kempen³ - H. M. Cuppen¹ - C. Brinch¹ - J. K. Jørgensen⁴ - M. R. Hogerheijde¹

1 - Leiden Observatory, Leiden University, PO Box 9513, 2300 RA Leiden, The Netherlands
2 - Max Planck Institut für Extraterrestrische Physik (MPE), Giessenbachstrasse 1, 85748 Garching, Germany
3 - Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, MS 78, Cambridge, MA 02138, USA
4 - Centre for Star and Planet Formation, Natural History Museum of Denmark, Øster Voldgade 5-7, 1350 Copenhagen K., Denmark

Received 2 February 2010 / Accepted 2 April 2010

Abstract
Context. Methanol has a rich rotational spectrum providing a large number of transitions at sub-millimetre wavelengths from a range of energy levels in one single telescope setting, thus making it a good tracer of physical conditions in star-forming regions. Furthermore, it is formed exclusively on grain surfaces and is therefore a clean tracer of surface chemistry.
Aims. Determining the physical and chemical structure of low-mass, young stellar objects, in particular the abundance structure of CH₃OH, to investigate where and how CH₃OH forms and how it is eventually released back to the gas phase.
Methods. Observations of the Serpens molecular core have been performed at the James Clerk Maxwell Telescope using the array receiver, Harp-B. Maps over a 4 $.\mkern-4mu^\prime$ $5 \times 5$ $.\mkern-4mu^\prime$ 4 region were made in a frequency window around 338 GHz, covering the 7_K-6_K transitions of methanol. Data are compared with physical models of each source based on existing sub-millimetre continuum data.
Results. Methanol emission is extended over each source, following the column density of H₂ but showing up also particularly strongly around outflows. The rotational temperature is low, 15-20 K, and does not vary with position within each source. None of the Serpens Class 0 sources show the high-K lines seen in several other Class 0 sources. The abundance is typically 10^-9-10^-8 with respect to H₂ in the outer envelope, whereas ``jumps'' by factors of up to 10²-10³ inside the region where the dust temperature exceeds 100 K are not excluded. A factor of up to $\sim$ 10³ enhancement is seen in outflow gas, consistent with previous studies. In one object, SMM4, the ice abundance has been measured to be $\sim$ $3 \times 10^{-5}$ with respect to H₂ in the outer envelope, i.e., a factor of 10³ larger than the gas-phase abundance. Comparison with C¹⁸O J= 3-2 emission shows that strong CO depletion leads to a high gas-phase abundance of CH₃OH not just for the Serpens sources, but also for a larger sample of deeply embedded protostars.
Conclusions. The observations illustrate the large-scale, low-level desorption of CH₃OH from dust grains, extending out to and beyond 7500 AU from each source, a scenario which is consistent with non-thermal (photo-)desorption from the ice. The observations also illustrate the usefulness of CH₃OH as a tracer of energetic input in the form of outflows, where methanol is sputtered from the grain surfaces. Finally, the observations provide further evidence of CH₃OH formation through CO hydrogenation proceeding on grain surfaces in low-mass envelopes.

Key words: ISM: abundances - ISM: molecules - stars: formation - ISM: individual objects: Serpens

1 Introduction

A long-standing goal of astrochemistry has been to determine the physical and chemical conditions prevailing in star-forming regions (e.g., van Dishoeck & Blake 1998). In this respect, different molecules act as tracers of different physical components, all depending on their formation history, their abundances, their chemical properties, etc. To effectively trace physical conditions such as density and temperature over the large range of values found in star-forming regions over the time-scale of star-formation, it is of great importance to have as many independent tracers as possible. Methanol (CH₃OH), with its rich rotational spectrum, is an excellent candidate tracing both temperature, density, grain surface formation and energy injection simultaneously during all phases of the early stages of stellar evolution.

CH₃OH is a slightly asymmetric top molecule with numerous rotational transitions observable at millimetre- and sub-millimetre wavelengths. Because of the large number of transitions observable in a single frequency window it is possible to obtain a coherent data set very efficiently, making methanol a very suitable tracer of physical conditions, in particular in low-mass star forming regions where the emission is optically thin. Moreover, since the molecule is a slightly asymmetric top molecule, it traces very efficiently both density and temperature (e.g., Maret et al. 2005; Jørgensen et al. 2005b; Leurini et al. 2007).

Methanol forms exclusively on ice-covered dust grain surfaces primarily through hydrogenation of CO (Watanabe & Kouchi 2002; Fuchs et al. 2009). Observations of interstellar ices show that methanol is indeed a prominent ice component, with abundances of up to almost 30% with respect to solid-state H₂O or a few $\times$ 10^-5 with respect to gas-phase H₂ (e.g., Pontoppidan et al. 2004; Dartois et al. 1999; Gibb et al. 2004). In contrast, pure gas phase reactions produce negligible CH₃OH abundances of less than 10^-10 (Garrod et al. 2006). The question that naturally arises is how methanol desorbs from the surface of a dust grain to be observed in the gas phase. Is it through thermal heating of the entire grain, or is it through non-thermal desorption, where cosmic rays, UV-photons or exothermic reactions provide local heating of the grain? The former mechanism is at play close to young stellar objects (YSOs), in the inner-most part of the molecular envelope where the gas temperature exceeds 100 K (van der Tak et al. 2000; Maret et al. 2005; Ceccarelli et al. 2000; Jørgensen et al. 2005b; van Dishoeck et al. 1995; Schöier et al. 2002) and in outflows where hot gas sputters the icy mantles (e.g. Bachiller et al. 1995; Bachiller & Pérez Gutiérrez 1997). This mechanism allows for an effective methanol enrichment of the environment and abundances are typically in the range of 10^-7 to 10^-6. The non-thermal mechanism dominates in cold, dark clouds and the outer parts of molecular envelopes (Herbst & Cuppen 2006; Hasegawa & Herbst 1993; Garrod et al. 2007; Öberg et al. 2009a). Here, reported abundances typically have values of 10^-10 to 10^-8. Hence, methanol also acts as a tracer of energetic processes in star-forming regions.

So far most studies have concentrated on spectra at a single position or at most a few around them. Recently, large-scale mapping of weak molecular lines has become very efficient with the advent of array receivers such as the 16 pixel Harp-B receiver on the James Clerk Maxwell Telescope (JCMT). This allows for a direct study of the entire protostellar system (primarily envelope and outflow) on scales of several arcminutes at 15 $^{\prime\prime}$ resolution and for determination of density, temperature and energy input into the system. These observations will eventually be compared directly to observations of another important grain surface product, H₂O, to be done with the Herschel Space Observatory. By mapping the entire region, comparison with the different Herschel-beams (9 $^{\prime\prime}$ -40 $^{\prime\prime}$ ) will be straight-forward.

The Serpens molecular core (also known as cluster A) is located at a distance of $230 \pm 20$ pc, following the discussion in Eiroa et al. (2008). The Serpens molecular core consists of several deeply embedded sources, of which at least four are identified as containing protostars (Wolf-Chase et al. 1998; Hogerheijde et al. 1999), SMM1, SMM3, SMM4 and S68N. Large-scale continuum-emission studies have been performed to quantify the spectral energy distribution of all sources in order to classify their evolutionary stage as well as the dust properties of the molecular envelopes surrounding each source (e.g., Davis et al. 1999; Hurt & Barsony 1996; Williams & Myers 2000; Testi & Sargent 1998; Larsson et al. 2000; Casali et al. 1993), most recently with the Spitzer Space Telescope as part of the Cores to Disks legacy program (c2d; Evans et al. 2009; Harvey et al. 2007). These studies show that three of the sources (SMM3, SMM4 and S68N) have relatively low bolometric luminosities of $\sim$ 5 $L_\odot$ each, whereas SMM1 has a higher luminosity of $\sim$ 30 $L_\odot$ (e.g., Hogerheijde et al. 1999; Larsson et al. 2000). The mass of each system (envelope and star) is in all cases less than 10 $M_\odot$ . Recent interferometer observations by Choi (2009) show that SMM1 is a binary system with a projected separation of $\sim$ 500 AU. The binary SMM1b appears less embedded than the primary (SMM1a). This discovery has been refuted by Enoch et al. (2009) and van Kempen et al. (2009) who both resolve the disk around SMM1. Through detailed SED modelling, Enoch et al. (2009) finds a very high disk mass of $\sim$ 1 $M_\odot$ and that the inner parts of the envelope have been cleared out to distances of 500 AU.

The region has been studied extensively at millimetre (mm) and sub-millimetre (sub-mm) wavelengths in numerous molecular transitions (e.g., Wolf-Chase et al. 1998; McMullin et al. 1994; Hogerheijde et al. 1999; White et al. 1995; McMullin et al. 2000), however it was not included in the molecular surveys of isolated Class 0 and I objects in Perseus and Ophiucus (Maret et al. 2005; Jørgensen et al. 2005b,2004). The previous molecular studies conclude that SMM1, SMM3, SMM4 and S68N are all very similar to other young, low-mass stars with similar luminosities, such as IRAS 16293-2422 and NGC 1333 IRAS4A and 4B in terms of abundances of simple molecules that may be formed directly in the gas phase, e.g., HCO⁺, CS, HCN (McMullin et al. 2000,1994; Hogerheijde et al. 1999). In Serpens, little has been done to quantify excitation and gas-phase abundances of molecules predominantly formed on dust grain surfaces, like CH₃OH, even though several lines have been detected by McMullin et al. (2000,1994) and Hogerheijde et al. (1999).

More direct observations of grain surface products have been made by Pontoppidan et al. (2004), who mapped infrared absorption by molecules in the ice over a region extending 40 $^{\prime\prime}$ south of SMM4, but still located well within the molecular envelope. The primary ice constituents were found to be H₂O, CO (0.4-0.9 with respect to H₂O), CH₃OH (0.28 with respect to H₂O) and CO₂(0.3-0.5 with respect to H₂O; Pontoppidan et al. 2008). The solid-state CH₃OH abundance is one of the highest reported to date, both when compared to H₂O but also with respect to gas-phase H₂ ( $3 \times 10^{-5}$ ). At distances greater than 12 000 AU the CH₃OH-ice abundance drops beneath the detection limit, corresponding to $3 \times 10^{-6}$ with respect to H₂.

Besides the protostellar objects themselves, the region is permeated by large-scale outflows extending several arcminutes from the different sources with CO J=2-1 velocities ranging from $\pm$ 10-15 km s^-1 with respect to $\varv_{\rm LSR}=8-8.5$ km s^-1(Davis et al. 1999; Graves et al. 2010). Garay et al. (2002) observed the outflows from SMM4 and S68N in CH₃OH 3_K-2_K emission and inferred CH₃OH column densities of 1- $2 \times 10^{15}$ cm^-2, corresponding to molecular abundance enhancements of $\sim$ 50-330, depending on outflow position, consistent with studies of other outflows (e.g., Bachiller et al. 1998,1995).

Here, the first map of rotationally excited methanol in the Serpens Molecular Core is presented of transitions which cover the energy range of $E_{\rm up} \sim 65{-}115$ K. The paper is structured as follows. In Sect. 2 the observations are presented, and in Sect. 3 the observational results are provided along with radiative transfer modelling. Section 4 presents a discussion of the results, with a particular focus on the formation, desorption and excitation processes. Section 5 concludes the paper.

2 Observations

$\begin{figure} \par\includegraphics[width=15.2cm,clip]{14182fg1} \end{figure}$

Figure 1:

Integrated emission, $\int T_{\rm MB}~{\rm d}\varv$ , of the strong 7₀-6₀ A⁺ line at 338.41 GHz. Objects Serpens SMM1, 3, 4 and S68N are labelled. Offsets are in arcsec with respect to SMM1. Contours are at 3 $\sigma$ , 6 $\sigma$ , 9 $\sigma$ , etc. The units for colour are K km s^-1. The pixel size is 7 $.\!\!^{\prime\prime}$ $5 \times 7$ $.\!\!^{\prime\prime}$ 5. The lines indicate outflow directions, with dashed representing blue-shifted outflow emission, and dotted lines representing red-shifted emission. The full white line extending south of SMM4 depicts the location of the four stars used by Pontoppidan et al. (2004) to measure the CH₃OH-ice abundance. Shown are also sample spectra at different positions, illustrated by triangles, from a single spatial pixel and provided in each inset in units of arcsec. The abscissa is for frequency in units of GHz and the ordinate is for main beam temperature in units of K. All spectra have the same scale to ease intercomparison.

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Observations of the Serpens molecular core were performed on June 20-22 2008 with the James Clerk Maxwell Telescope (JCMT) on Mauna Kea, Hawaii. Observations were made of the 7_K-6_K rotational band of methanol ( $E_{\rm up} \sim 65$ -115 K) at frequencies ranging from 338 to 339 GHz using the Harp-B array receiver consisting of $4 \times 4$ individual receivers (Smith et al. 2003). The telescope was pointed at two different locations near Serpens SMM1 and two different locations near SMM4, see Fig. 1, covering a total extent of 4 $.\mkern-4mu^\prime$ $5 \times 5$ $.\mkern-4mu^\prime$ 4. Observations were also made of C¹⁸O, J=3-2 at 329.330 GHz in a similar fashion, so as to be able to compare methanol and CO emission. Observations were made in jiggle-mode to achieve full spatial Nyquist-sampling using the Harp4 jiggle-pattern over a $2\hbox{$^\prime$ }\times 2\hbox{$^\prime$ }$ region. The beam-size of the JCMT at 338.5 GHz is $\sim$ 15 $^{\prime\prime}$ and data were subsequently put on a map with a pixel-size of 7 $.\!\!^{\prime\prime}$ 5, i.e., one half beam-size to fulfill the Nyquist sampling criterion. The methanol observations were done using beam-switch with a throw of 180 $^{\prime\prime}$ in azimuth while the C¹⁸O observations were done using position switch to a clean position 1 $^{\circ}$ off. The weather at the time of the observations was good with $\tau(\rm 225~GHz)\le 0.1$ . Pointing and calibration were checked at regular intervals, and the calibration error is estimated to be $\lesssim$ 20% based on a comparison with standard calibration sources. Data were brought from the antenna temperature scale, T_A^*, to the main beam temperature scale, $T_{\rm MB}$ , by dividing with the main beam efficiency, $\eta_{\rm MB}$ , which is 0.60 for the JCMT at these frequencies. The spectral resolution of the CH₃OH spectra is 0.43 km s^-1, and the C¹⁸O spectra were rebinned to the same value.

The mean rms in the methanol spectra is 20 mK in 0.43 km s^-1velocity bins over the entire map. The 1 $\sigma$ noise level on integrated emission has been determined as $1.2~\sigma_{\rm rms}~\sqrt{FWZI \times \delta\varv}$ where the factor 1.2 accounts for the 20% telescope calibration uncertainty, $\sigma_{\rm rms}$ is the rms noise, FWZIthe estimated full width at zero intensity (taken to be 5 km s^-1) and $\delta\varv$ the velocity bin (0.43 km s^-1). The 3 $\sigma$ uncertainty is typically $\sim$ 0.1 K km s^-1 per spatial pixel, but increases near the edges of the map by a factor of 2-3.

Initial data reduction was done using the Starlink package. This consisted of putting the spectra on to a regular grid with pixel-size 7 $.\!\!^{\prime\prime}$ 5, subtracting linear baselines and co-adding all data-cubes. The Gildas package CLASS was used for subsequent analysis. Standard data reduction revealed emission in the off-position for a subset of the methanol observations, but it was possible to remove this emission due to two facts: (1) the off-emission never coincided with on-emission, i.e., no double-peaked or ``self-absorbed'' line profiles were observed. In general the velocity offset between emission and absorption lines was of the order of $\sim$ 5 km s^-1 compared to typical line-widths of 3-4 km s^-1 in the region where the off-emission was seen. (2) Data were recorded with a shared off-position, that is, even though the telescope jiggled on the on-position, no jiggling was done on the off-position. Therefore it was possible to recreate the off-emission in the strongest emission line at 338.409 GHz in the following way: first the strongest ``absorption'' line was fitted with a Gaussian profile, then an artificial spectrum was created assuming a rotational temperature of 15 K, which was added to each spectrum. The spectra were then analysed and no absorption features remained within the noise limit.

3 Results

In all spectra emission lines from the 7_K-6_Krotational band of methanol are detected both on and off sources. In the central parts of each of the four YSOs up to eight emission lines are detected originating from ten transitions. The strongest line, the 7₀-6₀ A⁺ line at 338.409 GHz, has a peak brightness temperature of up to 0.5 K. All line profiles are Gaussian, no line asymmetries due to outflow activity or infall are observed. The FWHMof the emission lines are $\sim$ 4-6.5 km s^-1, consistent with other observations of methanol line widths (e.g. Maret et al. 2005; Jørgensen et al. 2005b). Line widths change between objects, but remain constant within each object, i.e., line widths do not change with position within an envelope. In Fig. 1 an overview is provided of the integrated emission in the strong 7₀-6₀ A⁺line over the Serpens molecular core. The integration is numeric and has been done over the velocity interval -25 to +25 km s^-1with respect to $\varv_{\rm lsr}=8.0$ km s^-1. The four Class 0 objects, Serpens SMM1, SMM3, SMM4 and S68N (labelled in Fig. 1) are clearly seen. Representative spectra obtained at different positions sampling both YSOs, molecular envelopes and outflows are shown. Besides the four Class 0 objects, three distinct outflow knots are identified, SMM1-S, SMM4-W and SMM4-S. All of these bright knots coincide with outflow positions as seen through CO observations (e.g., Davis et al. 1999). Weaker structure is also seen in the map, for example an elongation of SMM1 in the east-west direction. This corresponds to the direction of a weaker CO-outflow (Davis et al. 1999). The structure around S68N is more complex with the source itself being elongated in the NW-SE direction. Around this source a compact CS outflow has been discovered at the same position angle as the elongation (Wolf-Chase et al. 1998). Weak emission is also seen around S68N in the north-south and east-west directions.

$\begin{figure} \par\includegraphics[width=8cm,clip]{14182fg2} \end{figure}$

Figure 2:

Spectra of Serpens SMM1, 3, 4 and S68N. The NGC 1333-IRAS2A spectrum is shown for comparison (Maret et al. 2005). Spectra at the three outflow positions, SMM1-S, SMM4-W and SMM4-S, are also shown. Lines identified in the CH₃OH 7_K-6_K band are marked. Spectra were obtained by averaging emission from the peak pixel with its eight neighbouring pixels, i.e., in a box of 22 $.\!\!^{\prime\prime}$ $5 \times 22$ $.\!\!^{\prime\prime}$ 5. The SMM1, 3, 4 and S68N spectra are shifted by +0.25, 0.5, 0.7 and 1.1 K, respectively, while SMM1-S, SMM4-W and SMM4-S are shifted by 2.4, 2.0 and 1.7 K.

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Representative spectra of the central parts of the four envelopes are shown in Fig. 2 where emission is averaged over $3 \times 3$ pixels (corresponding to 22 $.\!\!^{\prime\prime}$ $5 \times 22$ $.\!\!^{\prime\prime}$ 5 or 5600 AU $\times$ 5600 AU). In the following, results will be presented first for the central parts of each envelope followed by results for the extended emission in each envelope. Finally results will be presented for three strong outflow knots in the map, named SMM1-S, SMM4-W and SMM4-S.

Table 1: Integrated line intensities, $\int T_{\rm MB}\ {\rm d}\varv$ (K km s^-1) over the central 22 $.\!\!^{\prime\prime}$ 5 $\times$ 22 $.\!\!^{\prime\prime}$ 5 of each source^a and emission-weighted, average line-widths.

3.1 Emission from the central part of the envelopes

The emission lines arising from the central part of each envelope are fitted with Gaussian line profiles to obtain the integrated emission at higher accuracy. Results are tabulated in Table 1 along with the upper level energy, $E_{\rm up}$ , and line frequency. In the spectra presented in Fig. 2 the 3 $\sigma$ level is a factor of three lower, since they are each the average of nine spectra. Low-K lines up to K = 3 are clearly detected, but high-K lines are not seen. This is in contrast to other low-mass YSOs with similar luminosities and/or distances and evolutionary stages, such as IRAS 16293-2422 (e.g. van Dishoeck et al. 1995) and NGC 1333 IRAS2A (Maret et al. 2005).

$\begin{figure} \par\includegraphics[width=8cm,clip]{14182fg3} \end{figure}$	Figure 3: Rotational diagrams with data obtained from the four spectra shown in Fig. 2. The best-fit straight line is shown in each case as a dotted line. Error bars are for 1 $\sigma$ uncertainties.
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The integrated intensities are used to make rotational diagrams for each of the four objects. These are shown in Fig. 3. Within the uncertainty, the logarithm of the derived upper level column densities, N, divided by the statistical weights, g, fall on a straight line when plotted versus the upper level energy divided by the Boltzmann constant, $k_{\rm B}$ . No difference between A- and E-type methanol is found, thus the abundances are equal, x(E-CH₃OH) = x(A-CH₃OH). In the cold-temperature limit ( $T \sim 10$ K) the abundance ratio is expected to be E/A=0.69 whereas it is 1 at higher temperatures, and thus little or no difference in abundance is expected (e.g., Friberg et al. 1988). The derived rotational temperature for each of the four envelopes is low, 15-20 K, significantly lower than the rotational temperature of $\sim$ 80 K inferred for IRAS 16293-2422 and NGC 1333 IRAS2A (Maret et al. 2005; van Dishoeck et al. 1995). The estimated column densities are all of the order of $\sim$ 10¹⁴-10¹⁵ cm^-2. Results are tabulated in Table 2. Rotational temperatures and column densities are similar to those found by Maret et al. (2005) and Jørgensen et al. (2005b) for a larger sample of low-mass, Class 0 objects, with the exception of the two sources mentioned above.

3.2 Extended emission from the envelopes

To quantify the spatial distribution of methanol in each molecular envelope, the radial distribution of emission from the five strongest lines is plotted in Fig. 6. Methanol emission is extended in all envelopes, and the FWHM of emission is around 2-3 times the 15 $^{\prime\prime}$ beam. Extended methanol has previously been reported in the envelope of the isolated Class 0 object L483 (Tafalla et al. 2000) in the 2₀-1₀ A⁺ and 2_-1-1_-1 E lines ( $E_{\rm up} = 12$ -20 K), where it was found that the methanol emission traces total gas column density. To verify whether this is true for the Serpens envelopes, it is necessary to quantify the physical structure of the envelopes. This is done through a combination of dust continuum emission at 850 $\mu$ m as observed with SCUBA on the JCMT and modelling of the physical structure.

To obtain the absolute abundances, three different methods are used. First, the CH₃OH column density obtained from rotational diagrams is compared to the column density obtained from dust emission at 850 $\mu$ m in the same beam. Second, the CH₃OH column density from rotational diagrams is compared to the column density predicted from a physical model of each source. Third, a radiative transfer model is compared directly to the observed spectrum to constrain the abundance. Results are listed in Table 4.

Table 2: Rotational diagram results for the observed methanol emission.

3.2.1 Dust continuum emission

Table 3: Best fit D USTY model input parameters and results for the physical structure of the four molecular envelopes in Serpens.

It is possible to directly estimate the average column density over the central area of each envelope by assuming that the dust emission is optically thin, thermal emission at a single dust temperature, $T_{\rm d}$ :

$\displaystyle \bar{N}$	=	$\displaystyle \frac{S_\nu d^2}{\kappa_\nu B_\nu(T_{\rm d})A}$
	=	$\displaystyle 4.90 \times 10^{16} {\rm\ cm}^{-2}\ S_\nu({\rm Jy})~ d({\rm pc})^2 \left[ \exp \left(\frac{16.9~{\rm K}}{T_{\rm d}} \right) - 1 \right]\cdot$	(1)

Here $S_\nu$ is the continuum flux integrated over 22 $.\!\!^{\prime\prime}$ $5 \times 22$ $.\!\!^{\prime\prime}$ 5 at 850 $\mu$ m, d the distance to the object, $\kappa_\nu$ the dust opacity at 850 $\mu$ m taken from Ossenkopf & Henning (1994), $B_\nu$ the Planck function at a dust temperature $T_{\rm d}$ and A the total surface area, in this case $7.1 \times 10^{33}$ cm². Finally a gas/dust ratio of 100 is assumed.

Reduced data from the SCUBA Legacy archive have been used (Di Francesco et al. 2008) to estimate the integrated continuum flux at 850 $\mu$ m. An average dust temperature of 20 K was used following global estimates of the dust temperature over the entire Serpens molecular core of 20 K from Schnee et al. (2005). If the temperature changes to 10 K, the column density estimate is increased by a factor of 3.3, while if it is 30 K, the column density is decreased by a factor of 1.8.

By using a dust temperature of 20 K, the average column density over a 22 $.\!\!^{\prime\prime}$ 5 $\times$ 22 $.\!\!^{\prime\prime}$ 5 region is in the range of 1- $4 \times10 ^{23}$ cm^-2. This leads to CH₃OH fractional abundances in the range of 1- $20 \times 10^{-9}$ with respect to H₂, see below.

3.2.2 D USTY modelling of envelope properties

Since the dust (and gas) temperatures change near the YSOs, the CH₃OH emission can be further quantified through modelling of the physical parameters of the envelopes. This is done following Schöier et al. (2002) and Jørgensen et al. (2002), where the dust continuum emission is modelled with a spherically symmetric envelope with a power-law density structure heated from the inside by the protostar, using the 1D code D USTY (Ivezic & Elitzur 1997). Dust opacities tabulated by Ossenkopf & Henning (1994) are used for densities of 10⁶ cm^-3 and thin ice mantles (corresponding to the values in their Table 1, Col. 5). The central heating source is taken to be a black-body radiating at a temperature of 5000 K, but model results are not very sensitive to this parameter. The output from D USTY is dimensionless, so to make an absolute calibration it is necessary to do so against the absolute luminosity and a given distance of the source. The output can be in the form of a spectral energy distribution (SED) and a radial profile of continuum emission at a user-specified wavelength.

Only dust heating at temperatures below 250 K is considered (corresponding to a peak wavelength of $\sim$ 12 $\mu$ m). Thus there is a ``hole'' in the inner part of the envelope extending out to a radius, $r_{\rm in}$ , where no attempt is made to model the dust emission. The physical extent of the envelope is defined by the parameter $Y=r_{\rm in}/r_{\rm out}$ . The density profile of the envelope is described by a power-law such that $n(r) \propto r^{-p}$ . Three observational constraints are used following Jørgensen et al. (2002) to identify the best-fitting dust model: the SED and the spatial distribution of continuum emission as recorded by SCUBA on the JCMT at 450 $\mu$ m and 850 $\mu$ m, both available through the SCUBA legacy archive (Di Francesco et al. 2008).

SEDs were assembled from the literature, using data points from MIPS on the Spitzer Space Telescope, ISO-LWS and IRAS along with ground-based single-dish continuum measurements at sub-mm, mm and cm wavelengths. For this work, the SED database available at http://astro.kent.ac.uk/protostars/ proved invaluable (Froebrich 2005). A full table of SED points is included in Appendix A.

The reduced SCUBA continuum emission maps from the SCUBA legacy archive have been smoothed to equivalent beam sizes of 11 $^{\prime\prime}$ and 19 $.\!\!^{\prime\prime}$ 5 at 450 and 850 $\mu$ m, respectively (Di Francesco et al. 2008). Along with emission maps, maps containing the error on each pixel are also provided, facilitating error analysis. The radial profile of each object was compiled by considering the emission in annuli extending from the pixel containing the maximum value of emission. The maps were carefully checked, and directions containing contamination from other objects were avoided.

Three D USTY input values were varied: the physical size of the envelope, Y, the opacity at 100 $\mu$ m, $\tau(100~\mu$ m) and the power-law slope of the radial density profile, p. A small grid of simulations was calculated and the best-fit model for each envelope was found using a $\chi ^2$ method, following Jørgensen et al. (2002). The best-fit model parameters are listed in Table 3 along with physical parameters such as the extent of the envelope, the local density at the inner radius, the column density and the total envelope mass. The best-fit model predictions are overplotted on actual data in Fig. 4.

In general agreement between the modelled and observed properties are good, except in the case of the modelled 850 $\mu$ m radial profile of S68N. The model prediction is consistently a factor of 2-3 lower than observed values. Part of the reason is that since several sub-mm sources are present close to S68N, only emission from the NW direction is modelled here, implying that the uncertainty on individual data points is higher than in the case of SMM1, SMM3 and SMM4. In this particular direction there may still be contamination, and thus emphasis is placed primarily on modelling of the SED. Moreover, the radial emission profile at 450 $\mu$ m is much steeper than the 850 $\mu$ m profile, indicating that there may be more cold, ambient cloud material toward S68N. The radial profile obtained at 450 $\mu$ m is well reproduced by the best-fit D USTY model.

$\begin{figure} \par\includegraphics[width=8cm,clip]{14182fg4} \end{figure}$	Figure 4: D USTY modelling results of the molecular envelopes of SMM1, 3, 4 and S68N. The left panel shows the SEDs of all four objects, whereas the right panel shows the normalized radial dust emission profile as obtained with SCUBA (Di Francesco et al. 2008). Best-fit results are over-plotted as solid lines, and the values for the best-fit models are given in the right-hand panel.
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From the D USTY model it is possible to estimate the average column density over a region of 22 $.\!\!^{\prime\prime}$ $5 \times 22$ $.\!\!^{\prime\prime}$ 5 and compare this to the CH₃OH column density. The average column density is found to be $\sim$ ( $1.0 \pm 0.2) \times 10^{23}$ cm^-2. This leads to an abundance of $\sim$ $3 \times 10^{-9}$ with respect to H₂ for SMM1 and SMM3 to $\sim$ $30 \times 10^{-9}$ for S68N (see Table 4 for details).

3.2.3 R ATRAN simulation

In the following the abundance is constrained through direct radiative transfer modelling. This has been done using the code, R ATRAN (Hogerheijde & van der Tak 2000) in conjunction with molecular data from LAMDA (Schöier et al. 2005). This opportunity was used to update collisional data in the LAMDA database for methanol using newly released rate coefficients for collisions between para-H₂ and A- and E-type methanol up to and including J=9, corresponding to an upper level energy of $\sim$ 500 K (Pottage et al. 2004). The rate coefficients are given for temperatures from 5 to 200 K. The coefficients are not complete up to upper level energies of 500 K since they are limited to J< 10. In the case of A-type methanol with K=0, this corresponds to an upper level energy of $\sim$ 100 K. Data have been extrapolated so that they are complete up to an upper level energy of 385 K corresponding to the first torsional state. For the extrapolation only transitions between K-ladders and $\Delta J=1{-}5$ are considered. The collisional rate coefficients are found to be proportional to $\sqrt{T}/\Delta J$ which is used for the extrapolation (Leurini et al. 2007). Level energies and Einstein A-values are taken from the Cologne Database for Molecular Spectroscopy (CDMS; Müller et al. 2001).

The density and temperature profile of the D USTY modelling is used for the physical structure of the envelope. No effort is made to model the line widths, but instead a constant, turbulent line width of 3.0-5.0 km s^-1 is assumed, depending on source. This is not a measure of the actual turbulence in the region, but only a means to ensure that the modelled linewidth corresponds to the observed. For each source a small grid of R ATRAN models has been run with a so-called ``jump'' abundance structure. The jump was located at $T_{\rm dust} = 80$ K (R = 50-125 AU) with an increase in the abundance of a factor of 1-10³ corresponding to most CH₃OH evaporating off of the grains. When running the R ATRAN models, great care has been taken to ensure that the central region containing the jump is properly sampled. In order to do this the pixel-size is set to 0 $.\!\!^{\prime\prime}$ 2 (45 AU) and the central pixels were oversampled by a factor of 50.

A $\chi ^2$ method is then used to determine the best-fit model integrated emission compared to observed integrated emission. This is done separately for A- and E-type CH₃OH to examine relative abundances. No significant difference is found between A- and E-type CH₃OH abundances, thus confirming the results obtained from the rotational diagrams. All abundances are listed in Table 4. Diagrams illustrating the variation of $\chi ^2$ with inner and outer abundance are shown in Fig. 5. Here it may be seen that the inner abundance is not well constrained, and it is only possible to provide upper limits ranging from $2 \times 10^{-9}$ (SMM1) to $5 \times 10^{-7}$ (SMM3 and S68N). On the other hand, the outer envelope abundance is very well constrained for all sources and lies in the range of 10^-9 (SMM1) to greater than 10^-8 (S68N). The methanol enhancements, $x_{\rm in} / x_{\rm out}$ , are from $\lesssim$ 2-3 (SMM1) to $\lesssim$ 200 (SMM3). Due to the lack of high-Klines it is not possible to further constrain the inner abundance.

$\begin{figure} \par\includegraphics[width=12cm]{14182fg5} \end{figure}$

Figure 5:

Reduced $\chi ^2$ distribution as a function of inner and outer abundance for A- and E-type CH₃OH as well as the combined value. Contours are for 1, 2, 3, 4 and 5 $\sigma$ . The dotted line corresponds to the abundance derived using N(H₂) from D USTY modelling, and the dashed line is the abundance derived using N(H₂) directly from SCUBA dust continuum emission. The minimum $\chi ^2_{\rm red}$ is given in each panel.

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Table 4: Average total gas column densities and fractional abundances of CH₃OH.

3.2.4 Comparison of abundance measurements

The three methods for determining the abundance may be divided into the following categories:

1.: Direct observational abundance assuming LTE in terms of CH₃OH excitation and optically thin dust emission.
2.: Combined direct and model abundance, still assuming LTE in terms of CH₃OH excitation but modelling the dust emission with a range of temperatures.
3.: Modelling of the CH₃OH emission within a physical, spherically symmetric model with varying dust and gas temperatures and densities.

Despite the obvious differences and levels of complexity between the three methods, the results in terms of average methanol abundances are remarkably similar. Typically, variations are within a factor of 2-3.

In the following only results from the R ATRAN modelling will be discussed. Since this method takes the full density and temperature structure into account it will be the more accurate of the three as demonstrated for other molecules (e.g., Jørgensen et al. 2002; Hogerheijde & van der Tak 2000; Jørgensen et al. 2004).

3.3 Outer envelope abundance structure

In Fig. 6 the column densities as predicted by the D USTY modelling and the 850 $\mu$ m dust continuum emission radial profiles are overlaid. The methanol emission profiles follow both the dust emission and column density profiles very closely over scales from $\sim$ 5500 AU to greater than 12 000 AU. Because the distribution is independent of rotational line, the rotational temperature (corresponding to line ratio) is constant throughout the envelope and the methanol column density scales directly with the envelope column density, similar to the case of L483 (Tafalla et al. 2000). Thus, over this range of radial distances, the average CH₃OH gas abundance is constant. In the case of S68N the agreement between the observed and simulated radial profiles is not good since the simulation under-estimates the emission at larger radii. Furthermore, the outer envelope abundance as derived from rotational diagrams or from comparison with dust emission agrees to within a factor of 2 with the outer abundance as derived from the R ATRAN modelling.

$\begin{figure} \par\includegraphics[width=15cm,clip]{14182fg6} \end{figure}$

Figure 6:

Spatial distribution of methanol emission in the four objects, Serpens SMM1, 3, 4 and S68N. The integrated emission of the five lines 7-6 +0E, -1E, +0A, +1E and $\pm$ 2E is shown (black). The error-bars are for 1 $\sigma$ uncertainties. Overlaid is the dust continuum emission as obtained from SCUBA (red) and the D USTY dust continuum modeling column density (blue). All profiles have been normalized to 1. The normalization factor for the peak emission is shown in each diagram. The 3 $\sigma$ noise level is shown as a dashed line, and the grey, dashed line shows the beam profile.

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3.4 Emission from outflow positions

Methanol is detected along the outflows throughout the emission map (Fig. 1). In the following, focus will be placed on emission from three distinct knots labelled SMM1-S, SMM4-W and SMM4-S in Fig. 1. The elongated emission associated with S68N indicates that a compact shock is responsible for sputtering CH₃OH from the grain mantles into the gas phase. This outflow has already been observed in CS J=3-2 emission (Wolf-Chase et al. 1998). The line profiles associated with this outflow are symmetric and Gaussian in nature making an accurate disentanglement of the contributions from envelope and outflow difficult. Unlike the above mentioned outflow knots, emission is spatially coincident with the source position. For this reason the S68N outflow is not included in the following discussion.

To investigate the properties of each outflow knot, spectra are extracted from the map and rotational diagrams are made in the same manner as above (see Figs. 2 and 3). The intensity of the strong 7₀-6₀ A⁺ line is comparable to the emission from SMM4 in all three knots. The detected transitions and associated intensities are listed in Table 1. The lines are shifted by $\sim$ 1 km s^-1 with respect to each other and with respect to the source velocities. Line profiles are symmetric and Gaussian in nature, with no obvious line-wings. Nevertheless, methanol clearly traces the outflow activity associated with SMM1, SMM4 and S68N as seen in Fig. 7, whereas little emission is associated with SMM3. In Fig. 7 the contributions from red- and blue-shifted emission are estimated by integrating over the velocity intervals from -5 to 7 km s^-1 and 10 to 20 km s^-1, respectively. This is to be compared with the average source velocity, $\varv_{\rm lsr}=8.5$ km s^-1.

Results obtained from the rotational diagrams are tabulated in Table 2. The rotational temperature is $\sim$ 10-15 K, indicating sub-thermal excitation at all three outflow positions, as found typically also in other outflows because of the relatively low density compared with the central envelope (e.g., Bachiller et al. 1995). The column densities range from a few $\times$ 10¹⁴ cm^-2 (SMM1-S and SMM4-W) to $\sim$ $3 \times10^{15}$ cm^-2 (SMM4-S). To obtain accurate abundance estimates of methanol in shocked regions, it is again imperative to estimate the gas column density accurately. In this case ¹²CO J=3-2 data from the JCMT science archive, obtained in the context of the JCMT Gould Belt legacy survey, are used (Graves et al. 2010). The principle for obtaining the column density from ¹²CO in the shocked gas is that emission from the higher velocity line-wings is optically thin. This assumption has been shown to be valid for a number of molecular outflows (see e.g., Bachiller & Tafalla 1999, for a review). In Fig. 8 the line profiles are shown for the three outflow positions analysed here. Emission from SMM1-S and SMM4-W is blue-shifted, while emission from SMM4-S is red-shifted. The CO line-wings are not as pronounced as in other well-known outflow sources (e.g., Blake et al. 1995), but are slightly shifted (up to $\pm$ 5 km s^-1) with respect to a $\varv_{\rm lsr}$ of 8.5 km s^-1. This indicates that the flows may be caused by J-type shocks rather than C-type shocks (Hollenbach 1997). Molecular emission is expected to have a Gaussian velocity profile around the shock velocity in a J-type shock, whereas emission caused by C-type shocks is expected to show a ``classic'', triangular line profile. However, since the observed lines are only shifted by $\pm$ 5 km s^-1 at most, so the J-type shock speed would be lower than this. CH₃OH is also efficiently destroyed in the sputtering process in J-type shocks at velocities greater than 10 km s^-1. The actual CH₃OH enhancement may be lower in the outflows in Serpens compared to e.g., L1157, something which is also discussed for the case of NGC 2071 (Garay et al. 2000). Another possibility is that the flows are C-type shocks moving very close to the plane of the sky, in which case the line-wings will not be prominent. This is suported by SiO J=2-1 observations of SMM4, where the lines were also found to be narrow ( $FWHM \sim 5$ km s^-1; Garay et al. 2002). With the present data-set it is not possible to differentiate the two scenarios.

$\begin{figure} \par\includegraphics[width=7cm,clip]{14182fg7} \end{figure}$	Figure 7: Outflow emission in Serpens as traced by the CH₃OH 7₀-6₀ A⁺ line. Contours are for red- and blue-shifted outflow emission and are at 3 $\sigma$ , 6 $\sigma$ , 9 $\sigma$ , ... Crosses mark the positions of SMM1, SMM3, SMM4 and S68N.
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$\begin{figure} \par\includegraphics[width=7cm,clip]{14182fg8} \end{figure}$

Figure 8:

Comparison of outflow line profiles. For each outflow position, SMM1-S, SMM4-W and SMM4-S, line profiles of ¹²CO J=3-2 (red), C¹⁸O J=3-2 (blue) and CH₃OH 7₀-6₀ A⁺ (black) are shown. C¹⁸O and CH₃OH spectra have been multiplied by 3 and 25, respectively, for clarity. SMM4-S and SMM4-W spectra have been shifted by 8 and 20 K. The masks at the bottom indicate the velocity range over which ¹²CO emission is integrated to obtain the outflow column density.

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Emission was integrated over the velocity intervals given in Davis et al. (1999). From this the CO column density is calculated under the assumption that emission is optically thin and that the gas temperature is 100 K. The calculation of the column density is insensitive to the choice of temperature, as long as it is in the interval of $\sim$ 50-150 K. The calculation is more sensitive to the choice of velocity interval over which CO emission is integrated, as this may vary by up to a factor of 2, when changing the velocity interval with 1 km s^-1. The column density is then converted to total gas column density using a standard abundance ratio of CO:H₂of 10^-4:1 and results are compared to CH₃OH column densities to obtain an abundance. The integrated CO intensities, column densities and CH₃OH abundances are all tabulated in Table 5. The gas column density in all three outflow positions is $\sim$ 10²⁰ cm^-2 resulting in abundances of $\sim$ 1- $10 \times 10^{-6}$ with respect to H₂. Due to the uncertainties on the derived CH₃OH column densities and on the gas column density, the abundances should be seen as order of magnitude estimates. Compared to the envelope abundances of SMM1 and SMM4, this translates to methanol enhancements in the outflows of $\gtrsim$ 10³. This is similar to what is found in other outflows; for example, the enhancement for the L1157 blue lobe is of the order of $\sim$ 400 (Bachiller et al. 1995; Bachiller & Pérez Gutiérrez 1997). It should be noted, however, that the methanol line profiles are highly asymetric in the L1157 outflow as are the CO line profiles.

C¹⁸O is often used as a tracer of quiescent gas column density. If C¹⁸O J=3-2 emission is used rather than ¹²CO emission as above, the gas column density is increased by $\sim$ two orders of magnitude to $\sim$ 10²² cm^-2. This leads to a decrease in CH₃OH abundance and therefore also a decrease in the enhancement. Representing the other extreme, typical enhancements are of the order of 5-50 (see Table 5). Ideally, emission should be integrated over the same velocity interval for comparison, but in this case, part of the CH₃OH line overlaps with the ¹²CO profile, part of it overlaps with the C¹⁸O profile, which is why these two abundance measurements should be seen as extreme values.

Table 5: Gas column density, N(H₂) and CH₃OH abundance in outflow knots as determined from ¹²CO J=3-2 and C¹⁸O J=3-2 emission.

4 Discussion

$\begin{figure} \par\mbox{\includegraphics[width=9cm]{14182fg9a}\includegraphics[width=4.5cm]{14182fg9b} }\end{figure}$

Figure 9:

Density and temperature profiles of the SMM1 and SMM4 envelopes as obtained from D USTY modelling. The radial density profile is displayed in blue ( left axis) and kinetic dust temperature in red ( right axis). The profiles are shown for the SMM1 envelope (full line) and the SMM4 envelope (dashed line). The CO freeze-out zone, characterised by temperatures lower than 25 K and densities greater than 10⁵ cm^-3, is shown in dark gray, whereas the methanol evaporation zone (T > 80 K) is shown in light gray. To the right is a cartoon illustrating the differences between the envelopes surrounding SMM1 and SMM4. Both illustrations are to scale and the dark blue regions correspond to the CO freeze-out zones while red indicates CH₃OH evaporation zones. Note the much smaller CO freeze-out zone for SMM1.

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The inferred abundances are all larger than what can be produced by pure gas-phase reactions (e.g. Garrod et al. 2006). Thus the observed CH₃OH gas must be formed on grains and subsequently have desorbed. In the following, possible scenarios for methanol desorption and excitation are discussed. Finally speculations on the nature of the individual young stellar objects in Serpens are made.

4.1 CH $_{\sf 3}$ OH grain surface formation

Methanol is formed on the surfaces of interstellar dust grains through hydrogenation of CO, a mechanism which has been studied in detail in the laboratory and in theoretical models of surface chemistry (Watanabe & Kouchi 2002; Hiraoka et al. 2002; Fuchs et al. 2009). To form large amounts of CH₃OH, it is imperative that CO freezes effectively out onto (water-ice covered) dust grains. Toward several pre-stellar cores (e.g., B68, Bergin et al. 2002) and Class 0 objects (e.g., Jørgensen et al. 2005c) CO has been observed to freeze out very efficiently at temperatures lower than $\sim$ 20 K and densities greater than $\sim$ 10⁵ cm^-3. This ``catastrophic'' CO freeze-out has been observed directly through observations of CO ice abundances which show an increase in the amount of solid CO with respect to H₂O ice in the densest regions (Pontoppidan 2006). Through use of D USTY modelling discussed above it is possible to estimate the extent of the CO freeze-out zone in each of the Serpens Class 0 objects quantitatively, which is illustrated in Fig. 9. Here the predicted density and temperature profiles are shown as a function of distance from the protostar itself. The density profiles of all four envelopes are very similar, however SMM1 stands out in terms of temperature profile. Due to the higher luminosity (30 $L_\odot$ ) of SMM1 with respect to the other source luminosities ( $\sim$ 5 $L_\odot$ ), the envelope temperature is also higher throughout.

The zone over which CO freezes out in SMM1 is significantly smaller than that of the other sources, SMM3, SMM4 and S68N. In the case of SMM1, the present freeze-out zone extends from $\sim$ 1000-5000 AU whereas the other envelopes have freeze-out zones starting at a few hundred AU and extend out to the same distance as for SMM1 (see Fig. 9). This indicates that at present CO is not freezing out efficiently in the SMM1 envelope, so any efficient methanol formation has probably ceased at this point in time. The colder envelopes surrounding SMM3, SMM4 and S68N could still be forming CH₃OH.

In terms of observing methanol directly in the ice itself, Pontoppidan et al. (2004) studied a small region extending south of SMM4 from 4000 AU to 12 000 AU by observing the 3.54 $\mu$ m CH₃OH features in absorption against background and embedded stars. The extent is illustrated by the white line in Fig. 1. In this region the CH₃OH-ice abundance is constant at 28% with respect to water ice or $3 \times 10^{-5}$ with respect to gas-phase H₂. This corroborates the interpretation presented here, that the gas phase abundance of CH₃OH is low and constant out to 12 000 AU in the SMM4 envelope. Beyond this line the CH₃OH-ice abundance drops by at least an order of magnitude and Pontoppidan et al. could only determine upper limits. It is interesting to note that the location where the ice abundance drops is where one of the outflow knots starts (SMM4-S; see Fig. 1). Thus the reason for the drop is a combination of the envelope being more tenuous ( $n_{\rm H}< 10^4$ cm^-3) far from the protostar, so that CO does not freeze out very efficiently, while at the same time whatever methanol is in the ice is sputtered into the gas phase by the outflow.

Cuppen et al. (2009) have recently studied the formation of CH₃OH on ice surfaces using a Monte Carlo method, in which the gas-grain chemistry based on laboratory data is simulated microscopically over long time-scales. The limiting factors in producing methanol is the availability of both CO and H on the grain surfaces, and so results show that CO hydrogenates efficiently to form CH₃OH, especially at temperatures lower than 12 K where atomic hydrogen can be retained efficiently. After 10⁵ years CH₃OH may form up to 100 individual mono-layers on the grain, comparable to that of water ice. Hence, the ice abundance of methanol in the outer parts of the envelope will depend strongly on the temperature. Because the envelopes of SMM3, SMM4 and S68N are significantly colder than that of SMM1, they would still be actively producing methanol, which could explain the higher gas phase abundances (see Table 4).

Observations show a different behaviour of C¹⁸O at the center position of S68N compared with the center position of SMM1. Figure 10 presents C¹⁸O J =3-2 emission in colour and methanol emission from the 7₀-6₀ A⁺line overlaid as contours. The morphology of the C¹⁸O emission shows a peak toward SMM1, as expected for a warm envelope, and a ring of emission toward S68N. The C¹⁸O abundances towards the two central positions are measured to be 3 and $1 \times 10^{-8}$ respectively, based on integrated C¹⁸O intensities of 4.3 and 2.4 K km s^-1 and the gas column densities derived from dust continuum emission (Table 4). This is to be compared to a standard C¹⁸O abundance of $1.8\times10^{-7}$ for a normal abundance of CO/H ₂ = 10^-4 and an ¹⁶O/¹⁸O ratio of 550 (Wilson & Rood 1994). Thus, CO is depleted by a factor of $\sim$ 6 and 18 for the two sources as averaged over the entire envelope. For these two sources there is a clear anti-correlation between CO and CH₃OH gas phase abundances.

$\begin{figure} \par\includegraphics[width=6cm,clip]{14182fg10} \end{figure}$	Figure 10: Integrated C¹⁸O, J=3-2 emission ( $\int T_{\rm mb} {\rm d}\varv$ ) is shown in colour, with integrated CH₃OH 7₀-6₀ A⁺ emission overlaid as contours. The image is centered on Serpens SMM1 with S68N located to the north. Outflow directions are indicated by dashed (red-shifted) and dotted (blue-shifted) lines.
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To examine whether this anti-correlation is unique to Serpens or a general feature of embedded sources, the outer-envelope CH₃OH abundances of the sample of Maret et al. (2005) and Jørgensen et al. (2005b) was coupled with CO abundances for the same sources from Jørgensen et al. (2002) (see Fig. 11). The CO gas phase abundance averaged over the extent of the envelope is taken as a tracer of CO depletion in the sense that the total gas and ice CO abundance is assumed to be constant. For sources where the presence of a jump zone can reproduce the observed CH₃OH emission, only the outer abundance is plotted here. A typical uncertainty of 30% is assumed both for the CO and CH₃OH abundances. Except for three sources (L1157, L1448-I2 and L483) there is a correlation between the two abundances as illustrated by the value of the Pearson correlation coefficient of r = 0.70. The Serpens sources are characterized by the combination of low CO-abundance and high CH₃OH abundance. This result implies that the CH₃OH gas phase abundance is directly related to the current production of CH₃OH in the outer, cold parts of the envelope, and that any difference from source to source is due to a difference in the amount of CO frozen out onto the grains. Thus, not all solid CH₃OH is formed during the cold pre-stellar core phase, consistent with the lack of detected CH₃OH ice toward background stars behind quiescent dense clouds. This also implies that the lack of CH₃OH emission at normal cloud positions between the sources is because the density is lower, and hence the timescale for CO to freeze out is much higher, i.e., the absolute CH₃OH abundance will drop.

4.2 CH $_{\sf 3}$ OH desorption mechanism

Once methanol has formed on a grain surface it can desorb according to two different mechanisms, thermal and non-thermal desorption. In the first mechanism the entire grain is heated thermally (macroscopic grain heating), and the icy mantle evaporates entirely, releasing all adsorbed species into the gas phase. The ice mantles typically evaporate at grain temperatures of 30-100 K, depending on species. The other mechanism is non-thermal desorption, in which the ice mantle is ``heated'' on a microscopic (local) scale, either due to absorption of a single UV-photon (Öberg et al. 2009c), impact of a cosmic ray particle (Herbst & Cuppen 2006; Hasegawa & Herbst 1993; Léger et al. 1985), or the binding energy being released from the formation of a new molecule (Garrod et al. 2007) or sputtering in outflows (Jiménez-Serra et al. 2008).

$\begin{figure} \par\includegraphics[width=9cm]{14182fg11} \end{figure}$

Figure 11:

CH₃OH gas abundance versus CO gas abundance for a selection of Class 0 and I sources based on data and analysis from Maret et al. (2005); Jørgensen et al. (2005b); Schöier et al. (2002) and this work. The Serpens sources are in red and IRAS 16293-2422 and NGC 1333-IRAS2A are in blue. Sources for which only upper methanol limits exist are marked by arrows. The two dashed lines indicate the 1 $\sigma$ confidence limits of the power-law fit.

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4.2.1 Thermal desorption

In the case of methanol, the thermal evaporation temperature has been determined experimentally to 80-100 K (Green et al. 2009; Brown & Bolina 2007) as is also indicated in Fig. 9. The lower temperature corresponds to evaporation of a pure CH₃OH ice and the higher to a mix of CH₃OH and H₂O. Because CO freezes out on top of a water ice, CH₃OH is expected to be present in the same layer. Thus the desorption temperature should be close to that of a pure CH₃OH ice ( $\sim$ 85 K), which is slightly lower, but not much, than that of CH₃OH mixed with H₂O. This is also found to be the case experimentally (Bisschop 2007). Thus, for the thermal-desorption mechanism to be active, it is necessary that all grains are heated to greater than 80 K, i.e., close to the protostar itself. From the physical structure models above it is predicted that the radius at which $T_{\rm dust} > 80$ K is of the order of 50-100 AU or 0 $.\!\!^{\prime\prime}$ 2-0 $.\!\!^{\prime\prime}$ 4 for d=230 pc, depending on source, leading to a beam-dilution factor of 1500-5000. Methanol emission originating from very close to the protostar itself has previously been observed for two low-mass sources, IRAS 16293-2422 (d=125 pc; van Dishoeck et al. 1995; Schöier et al. 2002) and NGC 1333 IRAS2A (d=250 pc; Maret et al. 2005). Even though the regions have not been spatially resolved with single-dish data, it has been possible to infer the existence of ``hot cores'' based on observations of high-K lines (K > 3) and measured rotational temperatures of >80 K. This indicates that the emission arises in a compact, warm and dense region, consistent with it originating close to the protostar itself and also consistent with high-spatial resolution interferometer data (e.g., Jørgensen et al. 2005a,2007). For the sources presented here, it has only been possible to provide an upper limit on the inner abundance, which in most cases is a few $\times$ 10^-7 with respect to H₂. One notable exception is SMM1, where the upper limit on the inner abundance is close to the outer abundance, a result that will be discussed further below (Sect. 4.3).

4.2.2 Non-thermal desorption

Since the temperature in the outer envelope is significantly lower than 100 K, the primary desorption mechanism must be non-thermal. This is supported by the fact that the abundance only follows the column density, and does not appear to depend on temperature. No attempt is made to distinguish between the above mentioned mechanisms here. If desorption is induced by secondary UV photons from cosmic ray ionization of H₂ the gas phase abundance is expected to be 10^-4-10^-3 times the ice abundance (Öberg et al. 2009b,a). In the case of SMM4 where the CH₃OH-ice abundance is $\sim$ $3 \times 10^{-5}$ with respect to H₂ (Pontoppidan et al. 2004) the UV-induced desorption alone can account for a gas phase abundance of 10^-9-10^-8. This is remarkably close to the observed gas phase abundance of $\sim$ $2 \times 10^{-8}$ .

Garrod et al. (2007) modelled the release of CH₃OH from the grain surface into the gas phase by examining whether the release of binding energy would be enough to evaporate the molecule into the gas phase. They found that the fraction was probably in the range of 1-10%, but could not pin it down any further. In the case of SMM4, results presented here combined with ice observations indicate that much less than 1-10% is desorbed, since the gas/ice abundance is $\sim$ 10^-4. Results presented in Hasegawa & Herbst (1993) show that direct cosmic ray desorption is not an efficient desorption mechanism for tightly bound species like H₂O and CH₃OH when compared to the accretion timescale. In fact, they find that the difference between the two rates is of the order of 10⁴. Previous studies show that direct cosmic ray induced desorption is most efficient for volatile species (see, e.g., Roberts et al. 2007; Shen et al. 2004) and for species adsorbed on very small grains ( $r \leq 0.05~\mu$ m; Herbst & Cuppen 2006).

4.2.3 Shock-induced desorption

In outflows the main desorption mechanism is sputtering of the grain mantle, i.e., impacts of high-temperature gas molecules and atoms, primarily H₂ and He. This can in principle be compared to the direct cosmic ray desorption mechanism, except that the flux of H₂ and He is orders of magnitude higher and the impact energy is much lower. The efficiency of this desorption mechanism is clearly seen from the fifth column of Table 5, where the CH₃OH abundance in the outflow positions is compared to the ambient envelope abundance. In particular, the SMM4-S methanol outflow abundance is $\sim$ 10^-5 with respect to H₂, i.e., only a factor of 3 lower than the measured CH₃OH-ice abundance in a region located $\sim$ 15'' (4000 AU) to the north (see Fig. 1 and Pontoppidan et al. 2004). If the envelope ice-abundance in this region were also $3 \times 10^{-5}$ prior to the impact of the shock, this would indicate that one third or more of the CH₃OH ice is sputtered from the grain mantle. However, the measured gas-phase abundance as determined from ¹²CO emission is an upper limit as briefly discussed above. The true value of the abundance probably lies in the range of 10^-8 to 10^-6 where the lower limit is obtained from C¹⁸O emission.

4.3 The nature of the embedded YSOs in Serpens

Two low-mass YSOs have been confirmed observationally to have the same chemical characteristics as high-mass hot cores, IRAS 16293-2422 and NGC 1333-IRAS2A. These two sources are at the same evolutionary stage as SMM1 based on classical indicators, e.g., $T_{\rm bol}$ . The characteristics are: (1) a large number of detected, saturated, complex organic molecules; and (2) a high rotational temperature for methanol (>80 K). At the same time, neither of these two envelopes show signs of extended methanol emission (van Dishoeck et al. 1995, Kristensen et al. in prep.). IRAS 16293-2422 is a close binary system surrounded by a circum-binary envelope. The inner parts of this envelope are passively heated to temperatures >80 K, which, along with small-scale shocks impinging on the inner wall of the envelope (Chandler et al. 2005), give rise to the observed hot-core signature. NGC 1333-IRAS2 is also a binary (possibly triple) system, but the projected separation is greater ( $\sim$ 30 $^{\prime\prime}$ ). It is believed that the same mechanisms are at play in NGC 1333-IRAS2A causing the hot-core signatures (Maret et al. 2005; Jørgensen et al. 2005b). In the following the Serpens sources, and in particular SMM1, will be compared to these two low-mass hot cores, and differences will be discussed.

There are several possible explanations for the lack of ``hot core'' characteristics in the Serpens sources which may be categorized in the following manner:

1.: Physical: No gas is present close to the source, or no hot gas is present.
2.: Chemical: Hot gas is present, but the methanol abundance is very low.
3.: Observational: Warm methanol is present close to the source, but either the extent is very small, or emission is optically thick.

Choi (2009) recently reported that SMM1 is a close binary with a projected separation of $\sim$ 500 AU. The primary would be the sub-mm source associated with SMM1 (SMM1a), while the binary (SMM1b) would be less embedded. SMM1b can be associated with a source observed by Spitzer at wavelengths shorter than 24 $\mu$ m, where SMM1a is not detected. If the projected distance is similar to the actual separation between the two sources, then this could have cleared the inner part of the envelope of gas, explaining the absence of hot gas close to the (sub-mm) source. However, both IRAS 16293-2422 and NGC 1333-IRAS2A have been shown to have inner holes or cavities similar in size to that of SMM1 (Jørgensen et al. 2005c; Schöier et al. 2002), therefore this cannot be the entire explanation.

Recent millimeter interferometry of SMM1 indicates that the region close to the protostar has been cleared of gas. Both Enoch et al. (2009) and van Kempen et al. (2009) report the detection of a resolved disk surrounding SMM1. The disk is unusually massive ( $\sim$ 1 $M_\odot$ ) and has a modelled radius of up to 300 AU (Enoch et al. 2009), while the inner 500 AU of the envelope have been cleared of gas. In such a dense disk, only the upper-most layers will be warm or hot, depending on the distance to the protostar, as the dust extinction grows rapidly towards the midplane of the disk. Thus, the column density of hot methanol will be very low. Through SED modeling of the disk, Enoch et al. (2009) estimate that the inclination is 15 $^{\circ}$ , i.e., nearly face-on. This is in conflict with observations of the 3.6-cm radio jet, which indicate that the outflow is moving very close to the plane of the sky (Rodriguez et al. 1989; Moscadelli et al. 2006). Moreover, the ¹²CO line profiles are very symmetric along the large-scale outflow, i.e., the molecular outflows are also moving close to the plane of the sky. This would indicate that the disk is seen close to edge-on. If so, then the beam-dilution will be very high implying that any hot part will not be detectable in our single-dish beam. The disk surrounding NGC 1333-IRAS2A is less massive compared to SMM1 ( $\sim$ 0.056 $M_\odot$ ; Jørgensen et al. 2009) and is viewed closer to face-on resulting in less extinction and lower beam dilution. This implies that the high-K emission observed in IRAS 16293-2422 and NGC 1333-IRAS2A is originating in the disk close to the protostar. The actual heating mechanism (passive heating or small-scale shocks) cannot be distinguished with the current observations.

If the inner part of the envelope has not been cleared out of warm gas or if the disk is seen face-on, then it is possible that the abundance of methanol is low. As has been shown by current observations, the CH₃OH gas-phase abundance is comparatively high in the outer parts of the envelopes, so to decrease the abundance in the inner part of the system, destruction of CH₃OH must be present. This destruction mechanism must be very efficient if it is to destroy all CH₃OH in the hot-core parts of the envelope, where the abundance is expected to rise to >10^-6 w.r.t. H₂. CH₃OH can be destroyed in the gas phase through direct reactions with other species, however the rate coefficients are typically low. An alternative mechanism of both the gas and the ice destruction is UV-dissociation. However, this destruction mechanism must also be at play in IRAS 16293-2422 and NGC 1333-IRAS2A and there is currently no reason why UV-photodissociation would be more efficient in Serpens sources than in the other two nor that the UV-field is enhanced in SMM1.

Finally, a low-mass hot core may be present in all of the Serpens sources, but not observable. This can be due to beam dilution or due to optical depth effects. The region over which methanol desorbs from the grain surface is expected to be $\sim$ 100 AU at most, and so beam dilution would be of the order of 10³. However, the same beam dilution would apply to at least NGC 1333-IRAS2A, which is located at a similar distance of 250 pc, and can thus not be used as an argument. The line optical depth has been calculated in the R ATRAN simulations, and is typically of the order of 0.1 or less for the transitions observed here, even for lines arising in the inner-most part of the envelope. The dust opacity at 338 GHz is less than 0.08 at all times, as estimated from the D USTY modelling.

Of the three explanations presented above the first is the more plausible if the distance is indeed 230 pc as assumed. Recent VLBA observations indicate that the distance may be closer to 415 pc (Dzib et al. 2010), in which case the third explanation is more plausible. The other two reasons can be disproved through comparison with IRAS 16293-2422 and NGC 1333-IRAS2A. However, only SMM1 has been suggested to have a massive disk, and it is also the source that resembles the two low-mass hot cores the most in terms of luminosity. The other sources (SMM3, SMM4 and S68N) have considerably lower luminosities by factors 4-10. Thus it may be that the hot-core regions around these sources are indeed much smaller and beam-diluted ( $\sim$ $5 \times 10^3$ ), comparable to several of the low-mass sources in the sample of Maret et al. (2005) and Jørgensen et al. (2005b). With the current observations only upper limits have been determined of the molecular abundance in the inner envelope of the lower-luminosity sources.

5 Summary

Maps of rotationally excited methanol in the Serpens Molecular Core have been presented. Emission arises from the molecular envelopes of four deeply embedded sources and their associated outflows. In particular, three outflow knots have been identified based on their strong methanol emission. Mapping shows methanol emission in all of the four envelopes to be extended out to ranges of $\sim$ 10 000 AU. The abundance is constant in the outer parts of the envelope with a value of 10^-9-10^-8, depending on source. The methanol abundance at outflow positions is enhanced by up to 2-3 orders of magnitude with respect to the ambient abundance. The measured envelope abundances are consistent with non-thermal desorption of solid-state methanol, through, for example, UV-photodesorption. At outflow positions the enhanced abundance may be explained by sputtering of the grain mantles. The symmetric, slightly shifted line profiles point to the outflows being either caused by J-type shocks or moving along the plane of the sky.

The CO gas abundance is found to be anti-correlated with the methanol gas abundance in the Serpens maps. This result has been extended to literature data of a large sample of other, similarly deeply embedded sources. The reason is that the more CO is frozen out from the gas phase, the higher the CO ice abundance, and this adsorbed CO is then converted to CH₃OH ice on the grain surface from where it desorbs non-thermally. The non-thermal desorption mechanism implies that the gas-phase abundance follows the solid-state abundance closely, something which has directly shown to be the case here. Thus, the differences in abundance between the four sources can be directly related to the current production of CH₃OH and reflects how much CO is frozen out now rather than in some possible colder past.

The Serpens sources do not contain the chemical signatures of low-mass hot cores such as IRAS 16293-2422 and NGC 1333-IRAS2A. In the case of SMM1, the more luminous of the Serpens sources and resembling most closely the two low-mass hot cores, the most likely explanation is that it harbours a massive disk which is seen close to edge-on. The other three Serpens sources are all lower in mass and luminosity, and here the absence of a hot-core signature could be ascribed to beam dilution, as also holds for the majority of the deeply embedded sources.

In conclusion, the CH₃OH emission is found to trace the following: (1) energetic input into cold gas, primarily through outflow interaction; (2) column density of cold gas in the outer envelope; (3) reactions and subsequent desorption of grain surface products.

Because water closely resembles methanol in the sense that it is exclusively formed on grains and it desorbs from grain surfaces at T > 100 K, it is expected that the abundance structure will resemble that of methanol. This is to be tested with upcoming water-observations of these sources as part of the Herschel Guaranteed Time Key Project ``Water in Star-forming Regions with Herschel'' (WISH).

Acknowledgements

Astrochemistry at Leiden Observatory is supported by a Spinoza prize and by NWO grant 614.041.004. The authors would like to thank the staff at the JCMT for technical help. Floris van der Tak is thanked for help with updating the LAMDA database and Karin Öberg for very stimulating disucssions. T.v.K. is grateful to the SMA for supporting his research at the CfA.

Appendix A: SED data points

Table A.1: SED points used for D USTY modelling.

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Footnotes

... Telescope: The James Clerk Maxwell Telescope is operated by the Joint Astronomy Centre on behalf of the Science and Technology Facilities Council of the United Kingdom, the Netherlands Organisation for Scientific Research and the National Research Council of Canada.

All Tables

Table 1: Integrated line intensities, $\int T_{\rm MB}\ {\rm d}\varv$ (K km s^-1) over the central 22 $.\!\!^{\prime\prime}$ 5 $\times$ 22 $.\!\!^{\prime\prime}$ 5 of each source^a and emission-weighted, average line-widths.

Table 2: Rotational diagram results for the observed methanol emission.

Table 3: Best fit D USTY model input parameters and results for the physical structure of the four molecular envelopes in Serpens.

Table 4: Average total gas column densities and fractional abundances of CH₃OH.

Table 5: Gas column density, N(H₂) and CH₃OH abundance in outflow knots as determined from ¹²CO J=3-2 and C¹⁸O J=3-2 emission.

Table A.1: SED points used for D USTY modelling.

All Figures

$\begin{figure} \par\includegraphics[width=15.2cm,clip]{14182fg1} \end{figure}$	Figure 1: Integrated emission, $\int T_{\rm MB}~{\rm d}\varv$ , of the strong 7₀-6₀ A⁺ line at 338.41 GHz. Objects Serpens SMM1, 3, 4 and S68N are labelled. Offsets are in arcsec with respect to SMM1. Contours are at 3 $\sigma$ , 6 $\sigma$ , 9 $\sigma$ , etc. The units for colour are K km s^-1. The pixel size is 7 $.\!\!^{\prime\prime}$ $5 \times 7$ $.\!\!^{\prime\prime}$ 5. The lines indicate outflow directions, with dashed representing blue-shifted outflow emission, and dotted lines representing red-shifted emission. The full white line extending south of SMM4 depicts the location of the four stars used by Pontoppidan et al. (2004) to measure the CH₃OH-ice abundance. Shown are also sample spectra at different positions, illustrated by triangles, from a single spatial pixel and provided in each inset in units of arcsec. The abscissa is for frequency in units of GHz and the ordinate is for main beam temperature in units of K. All spectra have the same scale to ease intercomparison.
Open with DEXTER
In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{14182fg2} \end{figure}$	Figure 2: Spectra of Serpens SMM1, 3, 4 and S68N. The NGC 1333-IRAS2A spectrum is shown for comparison (Maret et al. 2005). Spectra at the three outflow positions, SMM1-S, SMM4-W and SMM4-S, are also shown. Lines identified in the CH₃OH 7_K-6_K band are marked. Spectra were obtained by averaging emission from the peak pixel with its eight neighbouring pixels, i.e., in a box of 22 $.\!\!^{\prime\prime}$ $5 \times 22$ $.\!\!^{\prime\prime}$ 5. The SMM1, 3, 4 and S68N spectra are shifted by +0.25, 0.5, 0.7 and 1.1 K, respectively, while SMM1-S, SMM4-W and SMM4-S are shifted by 2.4, 2.0 and 1.7 K.
Open with DEXTER
In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{14182fg3} \end{figure}$	Figure 3: Rotational diagrams with data obtained from the four spectra shown in Fig. 2. The best-fit straight line is shown in each case as a dotted line. Error bars are for 1 $\sigma$ uncertainties.
Open with DEXTER
In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{14182fg4} \end{figure}$	Figure 4: D USTY modelling results of the molecular envelopes of SMM1, 3, 4 and S68N. The left panel shows the SEDs of all four objects, whereas the right panel shows the normalized radial dust emission profile as obtained with SCUBA (Di Francesco et al. 2008). Best-fit results are over-plotted as solid lines, and the values for the best-fit models are given in the right-hand panel.
Open with DEXTER
In the text

$\begin{figure} \par\includegraphics[width=12cm]{14182fg5} \end{figure}$	Figure 5: Reduced $\chi ^2$ distribution as a function of inner and outer abundance for A- and E-type CH₃OH as well as the combined value. Contours are for 1, 2, 3, 4 and 5 $\sigma$ . The dotted line corresponds to the abundance derived using N(H₂) from D USTY modelling, and the dashed line is the abundance derived using N(H₂) directly from SCUBA dust continuum emission. The minimum $\chi ^2_{\rm red}$ is given in each panel.
Open with DEXTER
In the text

$\begin{figure} \par\includegraphics[width=15cm,clip]{14182fg6} \end{figure}$	Figure 6: Spatial distribution of methanol emission in the four objects, Serpens SMM1, 3, 4 and S68N. The integrated emission of the five lines 7-6 +0E, -1E, +0A, +1E and $\pm$ 2E is shown (black). The error-bars are for 1 $\sigma$ uncertainties. Overlaid is the dust continuum emission as obtained from SCUBA (red) and the D USTY dust continuum modeling column density (blue). All profiles have been normalized to 1. The normalization factor for the peak emission is shown in each diagram. The 3 $\sigma$ noise level is shown as a dashed line, and the grey, dashed line shows the beam profile.
Open with DEXTER
In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{14182fg7} \end{figure}$	Figure 7: Outflow emission in Serpens as traced by the CH₃OH 7₀-6₀ A⁺ line. Contours are for red- and blue-shifted outflow emission and are at 3 $\sigma$ , 6 $\sigma$ , 9 $\sigma$ , ... Crosses mark the positions of SMM1, SMM3, SMM4 and S68N.
Open with DEXTER
In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{14182fg8} \end{figure}$	Figure 8: Comparison of outflow line profiles. For each outflow position, SMM1-S, SMM4-W and SMM4-S, line profiles of ¹²CO J=3-2 (red), C¹⁸O J=3-2 (blue) and CH₃OH 7₀-6₀ A⁺ (black) are shown. C¹⁸O and CH₃OH spectra have been multiplied by 3 and 25, respectively, for clarity. SMM4-S and SMM4-W spectra have been shifted by 8 and 20 K. The masks at the bottom indicate the velocity range over which ¹²CO emission is integrated to obtain the outflow column density.
Open with DEXTER
In the text

$\begin{figure} \par\mbox{\includegraphics[width=9cm]{14182fg9a}\includegraphics[width=4.5cm]{14182fg9b} }\end{figure}$	Figure 9: Density and temperature profiles of the SMM1 and SMM4 envelopes as obtained from D USTY modelling. The radial density profile is displayed in blue ( left axis) and kinetic dust temperature in red ( right axis). The profiles are shown for the SMM1 envelope (full line) and the SMM4 envelope (dashed line). The CO freeze-out zone, characterised by temperatures lower than 25 K and densities greater than 10⁵ cm^-3, is shown in dark gray, whereas the methanol evaporation zone (T > 80 K) is shown in light gray. To the right is a cartoon illustrating the differences between the envelopes surrounding SMM1 and SMM4. Both illustrations are to scale and the dark blue regions correspond to the CO freeze-out zones while red indicates CH₃OH evaporation zones. Note the much smaller CO freeze-out zone for SMM1.
Open with DEXTER
In the text

$\begin{figure} \par\includegraphics[width=6cm,clip]{14182fg10} \end{figure}$	Figure 10: Integrated C¹⁸O, J=3-2 emission ( $\int T_{\rm mb} {\rm d}\varv$ ) is shown in colour, with integrated CH₃OH 7₀-6₀ A⁺ emission overlaid as contours. The image is centered on Serpens SMM1 with S68N located to the north. Outflow directions are indicated by dashed (red-shifted) and dotted (blue-shifted) lines.
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In the text

$\begin{figure} \par\includegraphics[width=9cm]{14182fg11} \end{figure}$	Figure 11: CH₃OH gas abundance versus CO gas abundance for a selection of Class 0 and I sources based on data and analysis from Maret et al. (2005); Jørgensen et al. (2005b); Schöier et al. (2002) and this work. The Serpens sources are in red and IRAS 16293-2422 and NGC 1333-IRAS2A are in blue. Sources for which only upper methanol limits exist are marked by arrows. The two dashed lines indicate the 1 $\sigma$ confidence limits of the power-law fit.
Open with DEXTER
In the text

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