The literature was searched for determinations of dust scattering properties in objects possessing Milky Way interstellar dust. Astrophysical objects which satisfy this constraint are reflection nebulae, dark clouds, and the DGL.
For inclusion in this review, each study had to satisfy four criteria. These criteria are:
The studies satisfying the first three criteria are listed in Table 1, separated by astrophysical object studied. These tables give the study reference, a brief description, a model code, and whether the study satisfied the fourth criteria and, as such, was included in Figs. 1 - 4. Each model code is explained in Table 2 where the method of calculation, sources, and dust geometry are summarized. Ideally, the model used to interpret the observations of a specific object would include realistic illuminators (location and spectrum), a realistic dust distribution, and calculate the full multiple scattering of photons. This ideal is unlikely to be fully met by any specific model, but models which come closest have the best chance of producing good dust scattering properties. The original study reference should be consulted for the full details of each study.
Reference | Description | Model | Inc. |
Reflection Nebulae | |||
Witt et al. 1982 | NGC 7023; IUE 1200-3000 Å | RN1 | Yes1 |
& ground-based 3470-5515 Å | |||
Witt et al. 1992 | NGC 7023; UIT 1400 & 2800 Å | RN1 | Yes |
Witt et al. 1993 | NGC 7023; | RN1 | Yes |
Vogager 2 1000-1300 Å | |||
Gordon et al. 1994 | Sco OB2; 1365 & 1769 Å | RN2 | Yes |
Calzetti et al. 1995 | IC 435; IUE 1200-3100 Å & | RN1 | Yes |
ground-based B & V | |||
Burgh et al. 2002 | NGC 2023; FOT 900-1400 Å | RN1 | Yes |
Gibson et al. 2003 | Pleiades; WISP 1650 & 2200 Å | RN3 | Yes |
Dark Clouds | |||
Matilla 1970 | Coalsack and Libra dark | DC1 | Yes |
cloud; UBV | |||
Fitzgerald et al. 1976 | Thumbprint Nebula; B | DC1 | Yes |
Laureijs et al. 1987 | L1642; 3500-5500 Å | DC1 | Yes2 |
Witt et al. 1990 | Bok globule; 4690-8560 Å | DC1 | Yes |
Hurwitz 1994 | Taurus molecular cloud; | DC2 | Yes |
Berkeley UVX 1600 Å | |||
Haikala et al. 1995 | G251.2+73.3 cirrus cloud; | DC1 | Yes |
FAUST 1400-1800 Å | |||
Lehtinen & Mattila 1996 | Thumbprint Nebula; JHK | DC1 | Yes2 |
Diffuse Galactic Light | |||
Witt 1968 | ground-based 3600, 4350, | DGL1 | No3 |
& 6100 Å | |||
Mathis 1973 | ground-based 3600 & | DGL2 | Yes2 |
4350 Å | |||
Witt & Lillie 1973 | OAO-2 1500-4200 Å | DGL3 | No4 |
Lillie & Witt 1976 | OAO-2 1500-4200 Å | DGL2 | Yes |
Morgan et al. 1976 | TD-1 2350 & 2740 Å | DGL3 | Yes2 |
Toller 1981 | Pioneer 10 4400 Å | DGL4 | Yes |
Hurwitz et al. 1991 | Berkeley UVX 1625 Å | DGL5 | No5 |
Murthy et al. 1993 | Voyager 2 1050 Å | DGL6 | Yes2 |
Murthy & Henry 1995 | Berkley UVX & others | DGL6 | Yes2 |
Sasseen & Deharveng 1996 | FAUST 1565 Å | DGL7 | No6 |
Petersohn 1997 | DE 1 1565 Å | DGL8 | Yes |
Witt et al. 1997 | FAUST 1564 Å | DGL8 | Yes |
Schiminovich et al. 2001 | NUVIEWS 1740 Å | DGL9 | Yes |
1UV g determinations
not included, not enough radial data for unique g solution
|
The a and g values for the studies which satisfy all four criteria are plotted separate in Figs. 1 - 3 for reflection nebulae, dark clouds, and the DGL. In addition, predictions for different dust grain models are included in these figures (see Section 3.1. for model details). The results have been divided between object classes to highlight their differences. It would not be surprising to find real differences in the a and g values between object classes. For example, reflection nebulae and dark clouds possess, on average, larger dust grains than the DGL. This is seen from the different RV values measured for these objects as RV is a rough measure of the average grain size. Examining the results separately also allows for the impact of the different strengths and weaknesses of each object on the derived scattering parameters to be examined. The final reason to separate the results is to check if the assumptions in the modeling based on object type significantly affect the resulting scattering values. All of the a and g values have been plotted together in Fig. 4 to check the consistency of determinations between the three astrophysical object types.
Name | Method | Sources | Dust Geometry |
RN1 | Monte Carlo | single star | homogeneous sphere |
RN2 | Monte Carlo | multiple stars | homogeneous sphere |
RN3 | analytic | multiple stars | approximated |
single scattering | clumpy slab | ||
DC1 | Monte Carlo | MW ISRF & | homogeneous sphere |
specific stars | |||
DC2 | numerical int. | MW ISRF | 2D distribution |
DGL1 | analytic | Galaxy model | homogeneous slab |
DGL2 | numerical int. | MW ISRF | infinite cylinder |
n=8 scatterings | boundary condition | ||
DGL3 | analytic | constant | infinite slab |
DGL4 | numerical int. | star counts | non-homogeneous |
n=2 scatterings | |||
DGL5 | numerical int. | TD-1 star catalog | clumped dust |
DGL6 | numerical int. | SKYMAP catalog | dust based on |
HI survey | |||
DGL7 | Monte Carlo | star catalogs | dust based on |
HI survey | |||
DGL8 | Monte Carlo | TD-1 star catalog | dust cloud spectrum |
based on HI survey | |||
DGL9 | Monte Carlo | 3D TD-1 star catalog | dust cloud spectrum |
based on HI survey | |||
Figure 1. Determinations of the albedo and g in reflection nebulae are plotted versus wavelength. In addition, predictions from dust grain models are plotted for comparison. |
Figure 2. Determinations of the albedo and g in dark clouds are plotted versus wavelength. In addition, predictions from dust grain models are plotted for comparison. |
Figure 3. Determinations of the albedo and g in the DGL are plotted versus wavelength. In addition, predictions from dust grain models are plotted for comparison. |
Figure 4. The combined determinations of the albedo and g in reflection nebulae, dark clouds, and the DGL are plotted versus wavelength. The plot symbols are not identified and do not correspond to legends in previous figures, see Figs. 1 - 3 for information about specific studies. In addition, predictions from dust grain models are plotted for comparison. |