This is an introductory astronomy survey class that covers our understanding of the physical universe and its major constituents, including planetary systems, stars, galaxies, black holes, quasars, larger structures, and the universe as a whole.

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來自 Caltech 的課程

演变中的宇宙

369 個評分

This is an introductory astronomy survey class that covers our understanding of the physical universe and its major constituents, including planetary systems, stars, galaxies, black holes, quasars, larger structures, and the universe as a whole.

從本節課中

Cosmology and the Deep Universe

- S. George DjorgovskiProfessor

Astronomy

Well, let's move on then.

What do we do to get a little deeper than the distances of some kinds of

megaparsecs, which is what Cepheids can get you.

Now why do we want to do this?

Well, remember Hubble law is direct proportionality

between expansion velocity due to expansion of universe and the distance.

But what we measure is not just the Hubble velocity.

We always measure vector sum of galaxy's peculiar velocity, due to whatever

gravitational acceleration acts on it, and the actual cosmological velocity.

And now we know that those peculiar velocities could be as high as several

hundred kilometers per second.

Our own is 600 kilometers per second relative to microwave background.

So if all galaxies do that kind of thing, then that means you really need to

push much further out than 600 kilometers per second.

It turns out actually 300 is typical RMS, but let's say you want to go

to 7,000 kilometers per second of Hubble velocity just to minimize the effects.

Well, that's 100 megaparsecs, according to Hubble constant.

100 megaparsecs pretty far.

You can't see Cepheids that far away, so you have to do something else.

So you need to find some kind of objects that are really very bright so

they can be seen far away and/or very large, same reason.

And that's, in fact, how this was done.

So general trick here, and this applies as well in galactic astronomy,

is to find correlations between something that depends on distance,

like luminosity, and something that does not depend on distance.

In the case of galaxies it could be, say, velocity width.

And then you look at clusters of galaxies and plot those in an apparent sense, then

the relative shift is telling you what's the relative distance of one to the other.

And so if you can calibrate some of them absolutely,

then from that you can compute everything else.

So that's the generic idea behind distance indicator relations.

There is one very clever approach to this,

which was first invented by Ivan King, but nobody used it.

And then John Tonry reinvented it.

And it's like this.

You look at the galaxies and take their pictures, and so

they're a bunch of stars and they map onto your pixels.

The amount of flux in a given pixel is the number of star times the mean

luminosity per star.

Now you push that galaxy twice as far away, say.

Now there are four times as many stars in there.

And Poissonian variations always goes the square root of the number of stars.

So the Poissonian fluctuations and

mean fluxes per pixel do not scale equally with distance.

And because of the two different powers of distance, the ratio of the variance of

the RMS to the mean flux per pixel is direct function of the distance.

The further away a galaxy is,

the smoother it looks because there are more stars within each pixel.

And so this works beautifully for elliptical galaxies and

bulges, because there are no Cepheids in ellipticals.

Cepheids are young stars.

They're long gone from ellipticals.

And this was a very important approach to carry to the deeper Hubble flow.

So Cepheids work beautifully for spirals.

Surface brightness fluctuations are used for ellipticals.

We already talked about galaxy scaling relations, like Tully-Fisher for spirals,

absolute luminosity versus rotational speed, or fundamental plane if elliptic.

Also like radius versus a combination of surface brightness and

velocity dispersion.

And in the case of spirals,

the x-axis, the line is distance independent.

Y-axis in luminosity is distance dependent.

For fundamental planes the other way, y-axis does not depend on distance.

The x-axis is radius, it depends on distance.

And so we can use these correlations for galaxies and

clusters to find out how far they are.

But we need to calibrate the 0 point somehow.

And the way 0 point's calibrated for spirals is using Cepheids, and for

ellipticals it's using surface brightness fluctuations.

Now we can bypass this whole distance ladder and

push into really distant universe using two different methods.

One is using gravitational lensing and the other one is Synyaev-Zeldovich Effect,

about which we spoke when we talked about clusters of galaxies.

And how does this work?

Well, gravitational lensing you have some mass that splits image of some background

source.

And then if the background source varies in time,

quasars tend to vary, you can monitor all images of it and

see if variation that you see in one then repeats in a different one sometime later.

And the delay times the speed of light

gives you the difference in the light path.

So typically, let's say if you have two lensed images and

the light path is slightly different in length between one and the other, so

the geometry of this you can deduce from modeling the images on the sky.

And without necessarily knowing what the absolute distance is, but

just relative angles of things you can get from physical modeling.

So the difference in the light path is proportionate to the light path

themselves, right?

The whole thing scales up or

down depending what your choice of Hubble constant is.

And so if you can measure absolutely just the difference in the light path,

that nails down everything else.

So of course, the uncertainty is first the model, and then second you have to make

sure that variations that you observe are really just delayed version of each other.

But if you can do this reliably, and

it has been done with some kinds of gravitational lenses, then you have

a completely independent path path to Hubble constant deep out in Hubble flow.

At first this was giving little lower results than the nearby measurements, but

now I think there is convergence.

And again, Synyaev-Zeldovich Effect, which you probably recall is due to the fact

that clusters of galaxies are filled with X-ray gas.

So micro background photons get up-scattered,

scattering of those hot electrons, and

that creates a bump in the temperature or micro background.

By measuring that, you can infer how deep was the cluster.

So from X-ray measurement finding temperature, from micro background

measurements finding the magnitude, and that's directly proportional to the depth.

So that gives you the depths in megaparsecs.

Then you measure angular extent of cluster in the sky, and

different clusters will be different orientation and shape, but

on average the size in the sky should be the same as size along the line of sight.

And so therefore, you can use angular diameter test.