dark matter and dark energy

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Dark Energy & Dark Matter Shamit Kachru (Stanford and SLAC) LASER, Stanford, August 2012 Tuesday, August 7, 2012

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Shamit Kachru (Stanford Univ) at a LASER http://www.scaruffi.com/leonardo/aug2012.html

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Page 1: Dark matter and Dark energy

Dark Energy & Dark Matter

Shamit Kachru (Stanford and SLAC)

LASER, Stanford, August 2012

Tuesday, August 7, 2012

Page 2: Dark matter and Dark energy

Introduction

It was the burden of Newton to teach us that the same laws that we can infer from terrestrial experiments, also

apply in the heavens:

Tuesday, August 7, 2012

Page 3: Dark matter and Dark energy

Fast foward 250+ years:

We have learned a lot about the constitution and interactions of terrestrial matter!

Tuesday, August 7, 2012

Page 4: Dark matter and Dark energy

But, starting with Newton’s observation, we can infer that what we know about constitutes only a small fraction of

what exists:

In fact, Newtonian logic suffices to understand 1/4 of this. The other 3/4 requires Einstein.

Tuesday, August 7, 2012

Page 5: Dark matter and Dark energy

Dark Matter

Galaxies are massive, gravitationally bound systems that consist of stars and stellar remnants, gas and dust, and, as

it happens, a bit more.

There are in excess of 170 billion galaxies in the observable Universe. Telescopes capable of imaging distant galaxies

came online in the first quarter of the 20th century.Tuesday, August 7, 2012

Page 6: Dark matter and Dark energy

Fritz Zwicky and Vera Rubin were the first two to argue that there is more to typical galaxies than meets the eye:

Tuesday, August 7, 2012

Page 7: Dark matter and Dark energy

The flatness of the curve indicates that there is more matter present outside the luminous core of the galaxy.

Quantitative estimates, based by now on a bewildering variety of independent probes, indicate that there is five times more of this “dark matter” than there is stuff we

know about!

From indirect tests, as well as e.g. the Bullet Cluster event,Tuesday, August 7, 2012

Page 8: Dark matter and Dark energy

we know the dark matter interacts with “our” stuff very weakly. (Its self-interactions are also bounded).

Many candidates have been proposed for the composition of this stuff (and maybe more than contributes some

fraction):

Edward A. Baltz (KIPAC) XXXII SLAC Summer Institute Nature's Greatest Puzzles 8/2/04!

Dark Matter Candidates -A Terribly Incomplete Survey

Thermal Relics equilibrium !

at early timesSUSY neutralino !

SUSY gravitino!

Neutrinostandard model + sterile" #

right-handed

Non-thermal Relics !everything else

Axion

Primordial Black HolesPlanck mass and larger

???

This list is by no means complete I will focus on !

several classesSUSY is perhaps the favored source of dark matter candidates

Axions are the favored solution to the strong CP problem

Neutrinos are the least good candidate, but are known to actually exist

Primordial black holes are a possibility difficult to form!

There is a dirty little secret !if it's relevant it's more interesting than dark matter

Tuesday, August 7, 2012

Page 9: Dark matter and Dark energy

We aim to learn about it using either astrophysical “dark matter annihilation” events (e.g. in the center of

the galaxy):

or via production or direct detection here on Earth:

Tuesday, August 7, 2012

Page 10: Dark matter and Dark energy

Given that “our” 4% of the stuff gives rise to such diverse structures and consequences, it is perhaps reasonable to think that many things could be afoot in the dark sector.

Dark Energy

This still leaves us with a missing 75%. First of all, how do we know that? It is already perhaps surprising that we

could infer the existence of the dark matter, which interacts so very weakly with us.

The key to the discovery of dark energy lies back in the original observations of Einstein and Hubble.

Tuesday, August 7, 2012

Page 11: Dark matter and Dark energy

Einstein:

Gravitation is geometry. The geometry of space is fixed by the matter within it.

Hubble:

Space-time at the largest scales illustrates this!

Tuesday, August 7, 2012

Page 12: Dark matter and Dark energy

Expanding Universe encoded in “redshifts”:

Tuesday, August 7, 2012

Page 13: Dark matter and Dark energy

ds2 = !dt2 + a2(t)(dx2 + dy2 + dz2)

In a simple equation, the spatial slices are expanding in time in a way governed by a(t), the “scale factor”:

The dynamics of the Universe at large scales is then determined by how the various matter sources “tell” a(t)

to behave:

Tuesday, August 7, 2012

Page 14: Dark matter and Dark energy

* Very little mass leads to a Universe which expands forever, with the expansion slowed slightly by the

gravitational pull of matter.

* In contrast, above a critical amount, there is enough matter that its gravitational pull causes recollapse of the

spatial slices -- a “big crunch”.

What was completely unexpected in 1998, when the verdict came in, was the third possibility: a Universe that

not only continues to expand, but whose expansion accelerates!

Tuesday, August 7, 2012

Page 15: Dark matter and Dark energy

But this is what was found by a detailed study of the properties of distant Type IA supernovae.

Because of the way they arise, such supernovae are thought to be ~ “standard candles”.

Tuesday, August 7, 2012

Page 16: Dark matter and Dark energy

Old supernovae are brighter than they should be - because the expansion is accelerating!

Tuesday, August 7, 2012

Page 17: Dark matter and Dark energy

“Normal” matter -- stuff that behaves like dust particles -- and even photons, cannot make the Universe do this.

In fact, as nearly as we can tell, the accelerated expansion is caused by a small and positive “cosmological constant”

modifying Einstein’s theory -- an energy density of empty space.

Tuesday, August 7, 2012

Page 18: Dark matter and Dark energy

On the one hand, such a cosmological constant should not have been unexpected (though it was).

“Virtual” quantum particles, if nothing else, would be expected to generate a cosmological term in our best

theories.

This would be on top of any “classical” vacuum energy present in our vacuum.

Tuesday, August 7, 2012

Page 19: Dark matter and Dark energy

The best estimates we get from such quantum loops would suggest a “natural” size for the vacuum energy roughly

times larger than what we see!1060 ! 10120

How are we to understand this? We’re not sure yet.

Amazingly, the most conservative answer today (still untested) relies on vacuum selection occurring in a

complicated potential landscape:

Tuesday, August 7, 2012

Page 20: Dark matter and Dark energy

But to do justice to this subject would require further discussion of eternal inflation, string theory, and even

anthropic arguments; all would take us far afield, and we have no more time!

Such a potential landscape seems to arise naturally in string theory, one promising candidate for a theory unifying

gravity with other interactions:

Tuesday, August 7, 2012

Page 21: Dark matter and Dark energy

Thanks for your attention!

Shamit KachruDepartment of Physics

Stanford University and SLAC

http://www.stanford.edu/dept/physics/people/faculty/kachru_shamit.html

Tuesday, August 7, 2012