particle physics and cosmology (ppc) - are they...

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June 20, 2007 Particle Physics and Cosmology 1 Particle Physics and Cosmology Particle Physics and Cosmology (PPC) (PPC) - - Are they related? Are they related? - - Prof. Teruki Kamon and Prof. Bhaskar Dutta Department of Physics Texas A&M University REU Seminar (2007) June 20, 2007 1 June 20, 2007 Particle Physics and Cosmology 2 PPC are related!!! 2 Particle Physics and Cosmology June 20, 2007 Can particle physics help us understanding the Early Universe and the Big Bang? Today, we speak about the connection from a view point of upcoming collider experiment: Large Hadron Collider

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June 20, 2007 Particle Physics and Cosmology 1

Particle Physics and CosmologyParticle Physics and Cosmology(PPC)(PPC)

-- Are they related? Are they related? --

Prof. Teruki Kamonand

Prof. Bhaskar DuttaDepartment of PhysicsTexas A&M University

REU Seminar(2007)

June 20, 2007 1

June 20, 2007 Particle Physics and Cosmology 2

PPC are related!!!

2Particle Physics and CosmologyJune 20, 2007

Can particle physics help us understanding the Early Universe and the Big Bang?

Today, we speak about the connection from a view point of upcoming colliderexperiment: Large Hadron Collider

June 20, 2007 Particle Physics and Cosmology 33Particle Physics and CosmologyJune 20, 2007

http://ppc07.physics.tamu.edu/index.html

June 20, 2007 Particle Physics and Cosmology 4

HEP EXPERIMENT & THEORYHEP EXPERIMENT & THEORY[Collider Physics - CDF, CMS, International Linear Collider]

T. Kamon, P. McIntyre, A. Safonov, D. Toback [Neutrino Physics - MINOS, NOνA]

R. Webb [Dark Matter Detection - ZEPLIN, SIGN]

J. White[Phenomenology]

R. Allen, R. Arnowitt, R. Bryan, B. Dutta, D. Nanopoulos[String Theory]

K. Becker, M. Becker, D. Nanopoulos, C. Pope, E. Sezgin

ASTRONOMYASTRONOMY[Observational Astronomy]

N. Suntzeff, L. Wang, at least 2 more faculty members

Faculty Members and Research Areas

4Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 5

PPC Graduate and Undergrad. Students

… and students working on accelerator physics and string theory.

5Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 6

Thinking of Our Universe

6

My Universe

Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 7

Cosmic Microwave Background (CMB) was emitted when the Universe was only 380,000 years old.

The Most Distant Light

7Particle Physics and CosmologyJune 20, 2007

Message from the Universe

June 20, 2007 Particle Physics and Cosmology 8

4%

The 23% is still unobserved in the laboratory.. (This new matter can not be seen visually!)

We call this Cold Dark Matter..

Contents of the Universe

8Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 9

Examples of observations:

We know the dark matter exists.

Rotation curves of the galaxies

Collision of the galaxies

Existence of Dark Matter

9Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 10

4

3

2

1splitting normal matter and dark matter apart

– Another Clear Evidence of Dark Matter –(8/21/06)

Dark Matter(Gravitational Lensing)

Ordinary Matter(NASA’s Chandra X-ray Observatory)

Cosmic Collision of 2 Galaxy Clusters

10

time

Approximately the same size asthe Milky Way

Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 11

Dark Matter Sandwich

11

But we have a few clues. Let’s check what we know.

Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 12

What is Cold Dark Matter?

Can it be one of the known particles?Let’s check what we know.

It’s Doesn’t Matter.Right, it doesn’t shake hands with anyone easily. Two dark matter clusters (blue balls) are just passing each other.

It’s a Cold Matter.Yes, it is a “relativistically” slowly moving (“cold”) object.

12

4

It’s a Charge-less Matter.Right, it doesn’t respond to your flash light. This means it is a neutral object.

So, It’s a Cold Dark Matter.Right, it is a neutral and long-lived (stable) object.

Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 13

Thinking of Elementary Particles

13Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 14

Known Matter Particles

How many?

On

ion

Str

uct

ure

o

f M

atte

r

14Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 15

12 Particle-Zoo Animals

All masses in MeV.ANIMAL MASSES SCALE WITH PARTICLE MASSES

6 Types o

f Lept

ons

6 Types of

Quarks

The 12 elementary particles are fundamental building blocks of matter.

15Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 16

4 Zoo Keepers

NOTE : Graviton (G) ( not found) carries gravitational force.

g’s (gluons) strong forceQuarks experience them. Protons & neutrons are stick together.

γ’s (photons) electromagnetic forceQuarks, leptons (other than neutrinos) experience this force.

W’s (weak bosons) for weak forces Quarks, leptons experience this force.

16Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 17

June 20, 2007 Particle Physics and Cosmology 19

Heavy

Light

June 20, 2007 Particle Physics and Cosmology 20

Heavy

Light

Same force for all generationsAll reactions are explained by a single description (= theory).

Picture of Interactiond W + uW e ν

t W + bW e ν

17Particle Physics and CosmologyJune 20, 2007

W W

June 20, 2007 Particle Physics and Cosmology 18

[100 points] The Standard Model describes all these particles and 3 of 4 forces by paring two elementary particles. We have confirmed the existence of those in the laboratory experiments. Choose a candidate for the Dark Matter particle. Explain why.

CDM in The Standard Model?

June 20, 2007 Particle Physics and Cosmology 19

We need a new model.

No!Quarks, electron, muon, tau particles, and force carriers can not be the dark matter, since their interactions are stronger than what we expect.

Neutrinos can, but they have other problems.

X X XX X X

X X XX X X

XXXX

June 20, 2007 Particle Physics and Cosmology 20

We need an idea, based on a new symmetry.Supersymmetry or SUSY

Supersymmetrizing the Standard ModelNeutral-ino

This new charge-less (neutral) particle is the leading candidate for the dark matter.

New Idea

1) What is the new model? 2) Attractive?3) Can the neutralino be detected and consistent

with the dark matter content of the Universe?20Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 21

Mirror Reflection

Ferm

ilab

Bo

sela

b

21Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 22

Supersymmetric Reflectionγ

νe νµ ντ

e µ τ

But, one of them is neutralino. This is the lightest SUSY particle and stable.

Lots of new particles!!!!

Renamed as

“chi-o

ne zero

01χ~

02χ~

Renamed as

“chi-tw

o zero

,”

heavier than

chi-one ze

ro.

22Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 23

June 20, 2007 Particle Physics and Cosmology 20

Heavy

Light

SUSY decays can be described in the same way as the Standard Model.

Picture of Interaction (Again)t W + bW e ν

23Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 27

01χ~

~~Heavy

Light

The SUSY nature will be preserved through the entire decay chain. We graphically show this by yellow lines from the beginning to the ending.

tSUSY WSUSY + b

WSUSY χSUSY + e ν

WW

June 20, 2007 Particle Physics and Cosmology 24

YES. Physicists always dream about unification of all the forces.

Attractive?

We can construct a SUSY model with a stable neutralino to have the grand unification of the forces.

24Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 25

Particle Physics and Cosmology

8

pb 0.9

1

230

2

2

ann

0 ann

201

Mv

dxv

~h

.

fx

~

πασ

σΩ

χ

=

321

SUSY is an interesting class of models to provide a massive neutral particle (M ~ 100 GeV) and weakly interacting (WIMP).

SU

SY

SU

SY

CDM = Neutralino ( )CDM = Neutralino ( )01χ~

Ast

rop

hys

ics

Ast

rop

hys

ics

25Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 26

~0.0000001 seconds

When Were the Dark Matter Particles Created?

26

Now

CMB~380,000 years

(You = 20 yrs old)

(You = 4.8 hrs old)

Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 27

My Universe

Thinking of Dark Matter Detection

27Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 28

One promising way: In particle collisions

E = Mc2

Proton and ant-proton collision can produce the Standard Model particles like heavy top quarks (~180 times heavier than a proton!)

Physics Magic: PingPhysics Magic: Ping--pong balls pong balls Steel BallsSteel Balls

28Particle Physics and CosmologyJune 20, 2007

Tevatron Large Hadron Collider Linear Collider

June 20, 2007 Particle Physics and Cosmology 29

Large Large HadronHadron ColliderCollider (LHC)(LHC)

Two large international collaborations.

29Particle Physics and Cosmology

7 times powerful than the Tevatron

ATLAS

CMS

June 20, 2007

June 20, 2007 Particle Physics and Cosmology 30

““UndergroundUnderground”” ExperimentsExperiments

30Particle Physics and Cosmology

ATLAS

June 20, 2007

CMS(*)

(*) The TAMU group is a member of the CMS collaboration.

June 20, 2007 Particle Physics and Cosmology 31

CMS CMS -- Particle DetectorParticle Detector

31Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 32

Compact is a Relative

Term

CMS is significantly smaller than

ATLAS but heavier

Anatomy of CMSAnatomy of CMS

32Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 33

Collision as We Imagine Collision as We Imagine ……

33

We study blue and red dots and yellow lines to figure out what happens in the collision!

Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 34

Reconstruction as We Imagine Reconstruction as We Imagine ……

34Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 35

We have to extract this reaction out of many trillion pp collisions.

Key Reaction at the LHCKey Reaction at the LHC

35Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 36

11 2

2

2

2

max

1

01

02

102

τ

χ

χ

τ

χττ~

~

~

~

~M

M

M

MMM −−=

10 fb−1

LSOS

OS−LS

Mpeak = 47.1 GeV

Mmax(true) = 78.7 GeV

OS−LS counts with Mττ < 100 GeV:Top : 6 countsW+jets : 1 countSUSY : 125 counts

Phys. Lett. B 639 (2006) 46

Anatomy Anatomy –– Mass DistributionMass Distribution

36Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 37

OS

LS

OS−LS

Probing squark mass

Anatomy Anatomy –– Mass Distribution (2)Mass Distribution (2)

37Particle Physics and Cosmology

GOAL: Establish the technique before the experiment starts in 2008.

June 20, 2007

June 20, 2007 Particle Physics and Cosmology 38

We measure the masses (M) of the

particles at the LHC.

How do you know that the neutralinos (we will observe) at the collider are responsible for the dark matter content?

We calculate the dark matter content (Ω)in the new model of

the Universe.

1

230

0 ann

201 ∫

fx

~ dxv

~h

Ωχ

38Particle Physics and CosmologyJune 20, 2007

June 20, 2007 Particle Physics and Cosmology 39

0.1 201

=h~χΩ

0)(

0

40tan

GeV 350

GeV 210

0

1/2

0

>====

µ

β

sgn

A

m

m

GeV 114

GeV 151

GeV 260

GeV 830

01

02

====

χ~

τ~

χ~

g~

M

M

M

M We establish the dark allowed regions from the detailed features of the signals, and accurately measure the masses.

We calculate the relic density and compare with WMAP.

Work in progress

Example TranslationExample Translation

39Particle Physics and Cosmology

SUSYModel

June 20, 2007

With R. Arnowitt, B. Dutta, T. Kamon, D. Toback

June 20, 2007 Particle Physics and Cosmology 40

So far in the laboratories we have seen theparticles responsible for 4% of the universe.

The upcoming experiments (e.g., LHC) will tryto probe the nature of 23 % of the universe:dark matter.

Challenge:

73% of the universe is still a major puzzle.Not yet understood theoretically!

Conclusion

Particle Physics and Cosmology 40June 20, 2007