Photon radiation – signal definition Test of the SM – xsections, Afb, Rq’s

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Tests of the Standard Model and constraints on new physics from Fermion-pair production at LEP2 Georgios Anagnostou INP Demokritos Athens/Birmingham University HEP 2003 , Europhysics Conference in Aachen, Germany, July 2003

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Tests of the Standard Model and constraints on new physics from Fermion-pair production at LEP2 Georgios Anagnostou INP Demokritos Athens/Birmingham University HEP 2003 , Europhysics Conference in Aachen, Germany, July 2003. Outline. - PowerPoint PPT Presentation

Transcript of Photon radiation – signal definition Test of the SM – xsections, Afb, Rq’s

Page 1: Photon radiation – signal definition   Test of the SM – xsections, Afb,  Rq’s

Tests of the Standard Model and constraints on new physics from

Fermion-pair production

at LEP2

Georgios Anagnostou

INP Demokritos Athens/Birmingham University

HEP 2003 , Europhysics Conference in Aachen, Germany, July 2003

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• Photon radiation – signal definition

• Test of the SM – xsections, Afb, Rq’s

Constraints on new physics :

• Contact interaction

• Z’ bosons

• Low scale gravity

Outline

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EPS Aachen,July 2003

Photon Radiation – Radiative return to Z

• General feature of : often radiation of an initial state photon decreases effective collision energy √s’

•if √s’ close to Z peak more likely to interact significant enhancement of xsection - Radiative return to Z.

• Photon radiation complicates signal definition: Initial/Final state photons cannot be cleanly separated .

•LEP signal definition for reduced collision energy √s’ : mass of s-channel propagator with ISR-FSR interference subtracted so mass is unambiguous.

e e f f

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EPS Aachen,July 2003

Photon Radiation – Signal definition

Data sample divided into

- non-radiative √s’/√s > 0.85.

- inclusive events √s’/√s > 0.01.

• LEP combinations and new physics searches only for high energy sample.

• Radioactive events peak at √s’ ~ MZ used for independent beam energy measurement.

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LEP combinations

• Preliminary combinations for xsections σμμ, σττ, σhad and

asymmetries AFB(μμ), AFB(ττ) as well as dσ/dcosΘ’s and Rb/c, AFBb/c.

• Individual measurements performed with slightly different signal definitions corrections applied to derive results in common signal definition.

• Careful attention to correlated systematics systematic error broken down in parts according to correlations between channels, experiments.

• Averaging for xsections-asymmetries performed using BLUE technique.

Perhaps you already guess ..

In general good agreement between SM and data (χ2/d.o.f ~ 160/180).

Largest difference : Hadronic xsection slightly higher than expectation (~1.7σ).

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Cross-sections & Asymmetries

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EPS Aachen,July 2003

Differential cross-sections – μμ, ττ

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Heavy Flavours: Rb, AFBb, Rc, AFBc

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EPS Aachen,July 2003

Contact Interactions (I)

2

2, ,

( )( )(1 )eff ij i i j j

i j L R

gL e e f f

1

0

-Convenient parameterisation of new physics due to composite quark & leptons OR due to the exchange of heavy boson

with mX >> √s .

-Lagrangian has additional term:

- ηij describes chiral structure of the model

- Λ energy scale of new physics

- g unknown coupling

for e-e+ e-e+

otherwise

22

d σ 1( , ) ( , ) ε ( , ) ε , ε

dcosθA s t B s t C s t

-Fit ε (having set g2/4π=1)

- limits Λ+, Λ- correspond to constructive, destructive interference with SM.

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EPS Aachen,July 2003

Contact Interactions (II)

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EPS Aachen,July 2003

Extra Z’ Boson

- If SM embedded into a larger gauge group new heavy gauge boson, some of which will be neutral Z’.

-In general Z’ could mix with Z0, mixing parameterized by angle θE:

0'6 6sin cosE EZ Z Z

0

0'

cos sin

sin cos'

Z Z

Z Z

- Two additional gauge groups introduced.

- In general Z0’ will be a mixed state of Zx, Zy

-Example: E(6) GUT

E(6) SO(10) × U(1)χ

SU(5) × U(1)y

SU(3)C × SU(2)L × U(1)

Model Mixing

χ ΘE=0

ψ ΘE=π/2

- Also Sequential SM Z’ has same couplings to fermions as Z.

- Left Right symmetric model (LR) introduce additional SU(2)R

symmetry.

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Extra Z’ Boson (II) – Exclusion contours

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EPS Aachen,July 2003

Extra Dimensions - Low scale Gravity (I)

2(4), N PlG M 1 2

NV(r)= Gmm

r

1 22 1

( 4)

1V(r)

n nPl n

mm

M r

1 22

( 4)

1V(r)

n nPl n

mm

M R r

, r R

, r R

(1) & (2b) must look the same

2. (D=n+4) a)

1. (D=4)

b)

2 2(4) ( 4)

n nPl Pl nM M R

The two seemingly fundamental energy scales in nature MEW and MPl~GN

-1/2 have a ratio of 10-15 hierarchy problem.

• While ElectroWeak interactions have been tested experimentally at distances~MEW

-1, gravity tested only in the ~mm range.

•Assumption: MEW is the only fundamental short range scale in nature, even for gravity.

Assume,

n=1 R~1013cm

n=2 R~100μm-1mm

n=3.. 3

(4 ) (10 )Pl n EWM M GeV

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Extra Dimensions - Low scale Gravity (II)

Searches

Direct Indirect

*e e G f f e e G

2

4 8/ ( , ) ( , ) ( , )

s s

d d A s t B s t C s tM M

- SM interactions tested accurately up to MEW scale experimental constraint for SM particles not to propagate in extra dimensions only gravity does.

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Conclusions

• Results from 4 LEP experiments consistent and in good agreement with each other.

• Preliminary combined results for xsections, asymmetries and Rq's are in good agreement with SM expectations.

• Used to set limits to new physics depending on the model:

- contact interactions in the range 1.5-19.7 TeV.

- Z’ from 0.34-1.787 TeV.

- low scale gravity Ms > 1.2 TeV (λ=+1), 1.09 TeV (λ=-1).

• Final results now starting to appear. When available perform combinations and limit’s extraction again using same methods.

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Back-up slides

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EPS Aachen,July 2003

Differential cross-sections - Bhabhas

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Contact Interactions (III)

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Extra Dimensions - Low scale Gravity (III)