12 may 2004 alan barr uk atlas physics susy spin measurements with atlas alan barr “what else...

19
12 May 2004 Alan Barr UK ATLAS Physics SUSY Spin Measurements with ATLAS Alan Barr “What else could it possibly be?” “Don’t be so sure … hep-ph/0405052 “If it quacks like SUSY …” So … is it really supersymmetry?

Post on 22-Dec-2015

216 views

Category:

Documents


1 download

TRANSCRIPT

12 May 2004Alan Barr

UK ATLAS Physics

SUSY Spin Measurementswith ATLASAlan Barr

“What else could it possibly be?”

“Don’t be so sure … ”

hep-ph/0405052

“If it quacks like SUSY …”

So … is it really supersymmetry?

12 May 2004Alan Barr

UK ATLAS PhysicsExtended higgs sector(2 doublets)

(S)particle reminderSM SUSY

quarks (L&R)leptons (L&R) neutrinos (L&?)

squarks (L&R)sleptons (L&R)sneutrinos (L&?)

Z0

gluon

BW0

h0

H0

A0

H0

4 x neutralino

2 x chargino

AfterMixing

gluino

Spin-1/2

Spin-1

Spin-0

Spin-1/2

Spin-0

BinoWino0

Wino±

gluino

~

~

“Left squark” = scalar SUSY partner of

left quark

12 May 2004Alan Barr

UK ATLAS Physics

• Sparticle decays generate:– Missing ET (LSP)

– Jets (squarks/gluino)– Leptons (sleptons)

• “If we see these at LHC we have discovered SUSY”

• Not necessarily…

Scalar mass term (GeV)

Gaugin

o m

ass

term

(G

eV

)

Plot byD. Tovey

[RPC SUSY]1-year low-lumi mSUGRA reach

12 May 2004Alan Barr

UK ATLAS Physics

Universal Extra Dimensions

• TeV-scale universal extra dimension model• Kaluza-Klein states of SM particles

– same QN’s as SM– mn

2 ≈ m02 + n2/R2 [+ boundary terms]

– same spin as SM– KK parity

• Lightest KK state stable, and weakly interacting

• 1st KK mode pair-produced

• First KK level looks a lot like SUSY

hep-ph/0205314 Cheng, Matchev

“How to get fooled at the LHC”

Radius of extra dimension ~ TeV-1

KK tower of masses n=0,1,…

Dubbed “Bosonic Supersymmetry”

12 May 2004Alan Barr

UK ATLAS Physics

UED KK spectrum

1st excited KK level (example masses)

Example decay spectrum

Stable lightestKK particle(weakly interacting)

hep-ph/0205314 Cheng, Matchev

After adding boundary terms-> SUSY-like spectrum

Need to measure spins!

12 May 2004Alan Barr

UK ATLAS Physics

SUSY decay chain• Use mSUGRA

LHC point 5 as example

• Well studied in context of sparticle masses

• Nice leptonic signal at LHC

Spin-½, mostly wino Spin-0

Spin-½

Spin-0

Spin-½, mostly bino

Final state = jet + l+ + l- + ET

( + decay of other sparticle)

},{ el

12 May 2004Alan Barr

UK ATLAS Physics

Spin projection factorsIn rest frame of with +ve z-axis aligned with qL

Approximate SM particles as massless-> okay since m « p

Lq~Lq

Rl~

02~

Rl

1

0~ LqP

S

02~

12 May 2004Alan Barr

UK ATLAS Physics

Spin projection factorsIn rest frame of with +ve z-axis aligned with qL

Approximate SM particles as massless-> okay since m « p

Lq~Lq

Rl~

02~

Rl

1

0~ LqP

S

0

1~02 S

Σ=0

Spin-0

02~

12 May 2004Alan Barr

UK ATLAS Physics

Spin projection factorsIn rest frame of with +ve z-axis aligned with qL

Approximate SM particles as massless-> okay since m « p

(near) Rl

θ*p

SLq~

Lq

Rl~

02~

Rl

02~

12 May 2004Alan Barr

UK ATLAS Physics

Spin projection factorsIn rest frame of with +ve z-axis aligned with qL

**

**

1*

3*

cossin

sincos)sin()cos(ˆ

σp

Approximate SM particles as massless-> okay since m « p

(near) Rl

θ*p

SLq~

Lq

Rl~

02~

Rl

1

0~ LqP

S

0

1~02 S

Spin projection factorSpin-0

mql - measure

*210

2 sin~ Rl

02~

Σ=0

12 May 2004Alan Barr

UK ATLAS Physics

lnearq invariant mass (1)

m/mmax = sin ½θ*

Back to backin 2

0 frame

θ*

quark nearlepton

χ20

Phase space -> factor of sin ½θ*Spin projection factor in |M|2: l+q -> sin2 ½θ* l-q -> cos2 ½θ*

l+

l-

Phase space

Pro

bab

ility

)(sincos122 *212max2*2 lqqlqllq mppm pp

12 May 2004Alan Barr

UK ATLAS Physics

lnearq invariant mass (2)

squarkdecay

anti-squarkdecay

l+

l+

l-

l-

(Lepton from 2 decay only – not directly measurable)

Obvious asymmetry! Opposite asymmetry!

-> if same # squarks as anti-squarks effect cancels

0 1*

21sin

0 1*

21sin

12 May 2004Alan Barr

UK ATLAS Physics

How to measure?• lnearq shows nice charge asymmetry

– Excellent probe of spin of

• Experimental problems in measurement:– Can’t tell near lepton from far lepton

• Plot l+q and l–q instead -> contributions from both near and far

– Can’t tell quark jet from anti-quark• Sum of q and q-bar is measurable• pp collider -> get squark asymmetry from PDFs

02~

12 May 2004Alan Barr

UK ATLAS Physics

Production asymmetry

Peak near 0.1, 0.1Valence quarks

Parton distribution functionhas more q than q-bar for Bjorken x ≈ 0.1

-> pp collider produces more squarks than anti-squarks

x1 and x2 sampled by MC

(Twice as much for our point)

qg -> squark + gluino

12 May 2004Alan Barr

UK ATLAS Physics

Parton Level

ll

llA

difference/sum

l+l-

Experimentally measurable-> q and q-bar-> near and far leptons

Chargeasymmetry

Shape indicates that2

0 is spin-½

spin-0=flat

12 May 2004Alan Barr

UK ATLAS Physics

After detector simulation (ATLFAST)

l+

l-Change in shapedue to charge-blind cuts parton-level * 0.6

-> Charge asymmetry survives detector sim-> Same shape as parton level (but with BG and smearing)

detector-levelInvariant mass

Ch

arg

e a

sym

metr

y,

For cuts see C. Lester thesis

spin-0spin-½

Even

ts

12 May 2004Alan Barr

UK ATLAS Physics

Cross-checkNo asymmetry if spincorrelations turned off

• Monte Carlo is HERWIG (6.5)

• Can turn off spin correlations– distribution for

“scalar 20”

– consistent with flat– not consistent with

spin-½ 20 of

previous page (linearly increasing)

spin-½ -> 1)sin(2)(sin *21

~~*21 qqAA

spin-0 -> 0)(sin *21 A production asymmetry

spin-0=flat

12 May 2004Alan Barr

UK ATLAS Physics

Further evidence - slepton spin

• Dilepton invariant mass.– “Right-handed” slepton– l+ and l- are right handed– might expect

pronounced spin effects (as for lq distributions)

– none because slepton is scalar

• Scalar particle carrying lepton number– sounds like a slepton to

me!

Straightline distn

Shape after different-familysubtraction

Back-to-backin slepton frame

(phase-space)

12 May 2004Alan Barr

UK ATLAS Physics

Conclusions• Method for measuring spins of SUSY

particles at the LHC• Measure l±q invariant mass distributions

– equivalent to angular distributions in • Look for lepton charge asymmetry• Requires initial asymmetry in squark vs

anti-squark production– valence quarks in PDFs at x ~ 0.1

• Measure spin-½ nature of 20

• Also spin-0 slepton from mll

• Should be enough to kill “straw man” e.g. universal extra dimensions

*21sin