Stars and Baryonic Dark Matter IV
Isn't that also where they stop their analysis, at the 2.1 µm (K-band) point? Regardless, a simple straight line extrapolation on Figure 3 shows that the escape fraction is 100% by the time you get to 3 µm.
Dust opacity drops pretty sharply by 3 µm and beyond, but so does stellar emission. Dust opacity becomes large again around 10 µm because of silicate absorption features, and after that the opacity is a strong function of both wavelength and dust particle size (see, e.g.,
Optical Properties of Dust Grains in the Infrared: Our View on Cosmic Dust, M. Min; ASP Conference on "Cosmic Dust - Near and Far", 8-12 Sep 2008, published December 2009).
I worked with IRAC images out of the Spitzer Space Telescope, which has channels at 3.6 µm, 4.5 µm, 5.8 µm & 8.0 µm. The 3.6 µm channel is dominated by starlight, but stars are very weak at 4.5 µm and essentially invisible at 5.8 µm & 8.0 µm, and that's not due to dust opacity, it's due to the fact that there is essentially no starlight at wavelengths that long. But to get an idea of dust opacity that you can see, compare these two images:
- Axel Mellinger's Milky Way Panorama 2.0
- 2MASS Showcase: The Infrared Milky Way
Mellinger's panorama is a mosaic of about 3000 individual CCD images that is balanced for color & relative brightness to the human eye, which is most sensitive to light wavelengths where solar class stars are brightest, about 0.55 µm. In this image you can clearly see how well the dust concentrated along the plane of the Milky Way obscures the stars behind it.
The 2MASS ("2 Micron All Sky Survey") image is a composite all sky image where eyeball RGB corresponds to wavelengths in the infrared as 1.2 µm (blue), 1.6 µm (green) & 2.2 µm (red). The all sky orientation is the same as in Mellinger's image, so you can see & compare the same features in both images. The 2MASS image is all starlight & dust. As you can see, far more starlight is visible in the plane of the Milky Way in the 2MASS image than is the case in Mellinger's image.
In this case, the difference is due to far lower dust opacity at the infrared wavelengths. Starlight is far dimmer at the long 2MASS wavelengths, but the dust opacity is far lower than in visible wavelengths, and far more starlight directly escapes the galaxy at longer wavelengths. That's why Driver,
et al., are not specific about how they model starlight beyond 2.1 µm, there simply is not enough of it left anymore to bother their cosmological starlight in any significant way.
How would the luminosity increase relate to stellar mass?
But just looking at the standard main sequence mass (M) - luminosity (L) relationship (L = M3.5) I would guess that increasing the brightness by a factor of 2 would increase the implied mass by a smaller factor, about 1.2 (i.e., new stellar mass estimate = 1.2 x old stellar mass estimate).
The mass luminosity relationship for main sequence stars is extremely well established. The relationship is between the luminosity and the mass of the stars, not the number of stars. If I double L to 2L then I have to increase M by 1.2 so that M3.5 will also double to 2(M3.5) (a little diddling shows that a more precise number is 1.21903, close enough to 1.2 for the purpose of this discussion).
If you are talking in simple, general terms about mass & luminosity, that's it.
Looking
here, it seems that more massive stars are both bluer and much more luminous. For example, stars with twice the mass of the sun are 25 times as luminous, and significantly bluer. Stars 16 times the mass of the sun are 30,000 times as luminous.
This is important in light of this ...
If the galaxies are twice as bright, you could just as easily double the number of large stars in a galaxy.
This is one of the points I was criticizing. If we are specific about the wavelength dependence of the apparent brightness, then we must be equally specific about the class of stars were are going to increase because of the strong effect mass has on the wavelengths of peak brightness for stellar classes. Increase the number of small red stars and you increase the number of long wavelength photons, whereas if you increase large high mass stars you really pump up the short wavelength ultraviolet (UV) photons big time. In the absence of any claim that there is too much UV emission, you just can't diddle the high mass stars like that. Furthermore, the direct empirical relationship we have to work with is between stellar luminosity and stellar mass, not stellar number counts. Stick with what you
know and you can't go too far wrong. That's why I stick to the well known mass-luminosity relationship as a guide, and that's why I concentrate on lower mass stars, because I know there is no UV emission to justify the addition of high mass stars.
I will have more to say later but I have a chess tournament to get ready for now.