Part1 - Dark Matter Flashcards

(57 cards)

1
Q

what do we need to know to answer what universe we live in?

A

Ω0, which depends on the matter density of the Universe, ρ

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

ways to determine estimates of the matter density

A

visible stars in the milky way
galaxy rotation curves
application of the virial theorem
gravitational lensing
hubble diagram of standard candles
galaxy redshift and redshift-distance surveys

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

estimating matter density - visible stars in milky way

A

If we assume that all stars in the galaxy are of one solar mass, M⊙, then we can estimate the matter density to be:

p=NM⊙/volume of milkyway

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

In the early 1930s, Oort and Linblad showed that the Milky Way does not rotate as a rigid body, but…

A

differentially – i.e., the angular speed of stars around the galactic centre depends on their distances from it

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

The inner part of the disc rotates like

A

a rigid body: the speeds of stars are proportional to their distances from the galactic centre

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

The outer part of the disc is known as the

A

Keplerian part since the orbits approximately obey Kepler’s laws

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

The transition from rigid-body to Keplerian motion occurs at a distance

A

just inside the Sun’s distance from the galactic centre.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

A rotation curve is a plot of

A

rotation speed as a function of distance from the centre of the galactic disc

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

The mass outside the distance of a star from the centre of
the galactic disc has no effect on this star’s orbit hence

A

the total mass of the Galaxy
interior to, e.g., the Sun’s distance from the galactic centre can be estimated using Kepler’s third law

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

the observed rotation velocities are greater than those expected from the gravitational influence of the luminous stars alone, indicating

A

the presence of a dark matter halo surrounding the galaxy

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

what does it mean for a galaxy cluster to be virialised

A

reached a state of balance between their kinetic energy and potential energy such that 2K+U=0

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

virial mass estimate for a clutser

A

M=<v^2>Re/G

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

<v^2> is the 3D mean square peculiar velocity but in practice we measure

A

only the radial component of the peculiar velocity (deduced from the galaxy redshift)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

assuming a spherical cluster with an isotropic velocity distribution, <v^2>=

A

3<v_radial^2> = 3sigma^2

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

The use of the Virial theorem assumes that

A

clusters are spherically symmetric and in a relaxed equilibrium state. It is further assumed that galaxies can be seen as being in a fluid in hydrostatic equilibrium (HE) with random orbits acting as outward
pressure.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

Various methods exist to solve for M(< r) given the observables (σ^2
and the projected galaxy surface density), including:

A
  • Assuming that light traces mass, and estimating M/L.
  • Observing hot gas in X-rays, knowing that X-ray emissivity scales as ρ^2

these methods also depend on knowledge of Hubble’s constant

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
17
Q

what is gravitational lensing

A

A massive object acts as a lens that
bends the passage of light from a source object behind it. The result is the generation of images of the source object that can be distorted, magnified and / or brightened.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
18
Q

2 ways in which we can use lensing to deduce estimates of the matter density

A
  1. strong and weak lensing events
  2. microlensing
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
19
Q

strong and weak lensing events

A

light from distant galaxies is distorted by passage through an intervening cluster.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
20
Q

what is microlensing

A

where the mass of the bending object is too low for easy detection
of its effect on the light of the source object.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
21
Q

In microlensing, the expectation
is that the bending object will change position over

A

a relatively short timescale,
cosmologically speaking.

(so photometry over a period of time may be used to monitor changes in the source’s apparent brightness)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
22
Q

For relatively nearby objects the relation between apparent magnitude and log redshift is

A

linear

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
23
Q

relationship between apparent magnitude and log redshift for more distant objects

A

begins to curve (amount of curvature indicates the curvature of the universe)

24
Q

The large-scale distribution of galaxies in the Universe is far from uniform, due to

A

the influence of gravity causing structures in the galaxy distribution to grow as the Universe evolves.

25
the higher the matter density...
stronger the pattern of galaxy clustering.
26
If we also have redshift-independent information about the distance of the galaxies then we can
directly measure their line-of-sight peculiar velocity, which results from the gravitational pull of the surrounding matter distribution.
27
By studying the patterns of galaxy peculiar velocities we can also
estimate Ω0
28
nucleosynthesis
considering the relative amounts of the lightest elements, which we believe were manufactured during the first few minutes after the Big Bang
29
nucleosynthesis constrains
the density of baryons *does not make any statement on the density of non-baryonic matter*
30
CMBR
constrain very precisely both the baryonic and non-baryonic matter density
31
conclusive evidence for dark matter
Estimates of Ω0 from visible stars are a factor of about 100 smaller than estimates from galaxy clusters, large scale motions and gravitational lensing
32
is dark matter baryonic or non-baryonic?
Dark matter is simply matter that cannot be seen through telescopes, and it can be baryonic or non-baryonic.
33
evidence for dark matter also being between galaxies
Since the values of Ω0 from galaxy clusters are a factor of ∼ 10 greater than from galaxy rotation curves, it seems that dark matter is not only in galaxy halos, but also between galaxies.
34
The WMAP value for the averaged density parameter of all types of matter is consistent with that obtained from
studying gravitational effects in a variety of astrophysical systems
35
how much matter is baryonic?
only 16% the rest is non-baryonic
36
in the case where Ω0<1, we can expect a
fast decrease from Ω-1 to Ω-->0
37
due to the fast decrease, any value of Ω0 which is not approx 1 or approx 0 would
place us at a very special time
38
often assumed that Ω0=1 which requires
the existence of another unknown component in the universe
39
Baryonic matter is matter made up of
neutrons, protons (and electrons)
40
estimates of Ω0 from visible stars are a factor of about 100 smaller than
estimates from galaxy clusters, large scale motions and gravitational lensing
41
why does estimates of Ω0 from visible stars being factor of 100 smaller than other methods provides
conclusive evidence for the existence of dark matter
42
X-ray observations indicate a smooth distribution of
intra-cluster gas in galaxy clusters
43
the limits on Ωbh^2 are deduced from
the dependence of reaction rates on density and temperature in the early universe
44
if h=0.7, then Ωb is between
0.031 and 0.053
45
limits of 0.031 and 0.053 for Ωb are compatible with Ω0 from galaxy rotation curves but
fall well short of the limits on Ω0 from larger scales eg from CMBR
46
dark matter candidates - baryonic
1. gas clumps in galaxy halos and clusters 2. MACHOs 3. Low surface brightness galaxies
47
MACHOs
Massive compact halo objects such as 'Brown dwarfs' (failed stars), 'Jupiters' (cold planet-like objects)
48
dark matter candidates - non-baryonic
WIMPs primordial black holes
49
WIMPs
weakly interacting massive particles eg massive neutrinos, exotic particles
50
examples of exotic particles
axions, photinos, magnetic monopoles, wimpzillas
51
Note that if primordial black holes form before nucleosynthesis then they don’t
affect the limits on Ωb so are effectively non-baryonic
52
Non-baryonic dark matter interacts weakly with baryons and photons now, but
interacted more strongly (ie was more strongly coupled to them) in the early universe which was hotter and denser
53
hot non-baryonic dark matter
if non-baryonic matter was moving relativistically at the time of decoupling from baryonic matter
54
examples of hot dark matter
neutrinos and photinos
55
cold non-baryonic dark matter
moving non-relativistically at decoupling
56
57