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MCP checks for the H- 4l mass
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MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the – Possible single resonant peak mass shift (with.

Dec 28, 2015

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Donna Hubbard
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Page 1: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

MCP checks for the H-4l mass

Page 2: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Outline and work program

• The problems:– Higgs mass difference from the gg– Possible single resonant peak mass shift (with low stat)– M12 in the 2mu2e channel shifted

• MCP checks (to be finalized):– Muon absolute mass scale– Overall Momentum scale– Local misalignments– Per Event mass error

• Work program

Page 3: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

The main problem

Inconsistency between the two masses 2.7 s

Page 4: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Other “features” in the H-4l analysis

• Z-4 Leptons – Single resonant

Distributions

Apparent shift in the the single resonant mass spectra with standard analysis cuts

Fully relaxed analysis to increase stat: M34>0All Pt>4 GeVMass increased from 89.4 -> 90.4For 2011 we have MC without cutsMass DT = 91.0 ± 0.8 GeVMass MC = 91.1

Increasing stat

Mass increased from 89.4 -> 90.4

Page 5: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

M12 Distributions

Very good agreement on M12 with 4 mu

Disagreement in tails of M12 for 2mu2e events

Page 6: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

M12 in 2mu2e events

• Fit crystal-ball conv. BW• cbmean shift w.r.t. MC mass value• Diif = 0.8 ± 0.5

Page 7: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

MCP Checks: Absolute scale using Z events

• Template fit of the Z mass (DT and MC)

• Results given as Scale factors to be applied to the PDG mass value in different eta region.

• To be finalized using Z in different Pt ranges

Eta Region Scale Factors

-2.5 -2 1.0034

-2 -1.7 1.0005

-1.7 -1.05 0.9992

-1.05 1.05 0.9992

1.05 1.7 1.0004

1.7 2.0 1.0007

2.0 2.5 1.003

Eta Region Scale Factors

-2.5 -2 1.002-2 -1.7 1.003-1.7 -1.05 0.998-1.05 1.05 0.998

1.05 1.7 0.9971.7 2.0 0.9982.0 2.5 1.003

MC Data

Error on these numbers : Max 10-3

Page 8: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Z reconstruction different Pt regionsData-MC agree at the level of about 100 MeV over the full Pt rangeDisclaimer this is NOT a measurement of the Z mass as in the previous page so we are NOT looking at agreement between PDG value and fit.

Page 9: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

MCP Checks: Mass scale vs Pt• Reconstruct Z Mass for data and

MC as a function of leading muon Pt

• Plot difference DT-MC difference vs Pt for ID, MS and CB reconstruction

• Mean difference < 0.2% stable over data taking period and Pt.

• Same results on the other end cap and Barrel

• To be done– Enlarge the Pt coverage to lower Pt. – Cross check the results with J/Psi

and Y data.

Standalone

Combined

ID

End Cap A

Page 10: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

MCP Checks: Pt scale vs Pt• Plot difference between DT and

MC of the measured Pt in ID and MS and in ID and Cb

• Difference 100 MeV for Sa-ID stable over data taking period and Pt.

• Same results on the other end cap and on the barrel

• To be done– Enlarge the Pt coverage to lower Pt. – Cross check the results with J/Psi

and Y data.– Check charge dependent

distributions

Standalone

Combined

End Cap AData [PT(SA)-PT(ID)]–MC[PT(SA)-PT(ID)]

Data [PT(CB)-PT(ID)]–MC[PT(CB)-PT(ID)]

Page 11: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Checks with J/Psi and Y • Different studies done with

J/Psi and Y– Some small inconsistencies

between them to be understood

• General picture: – Also from J/Psi absolute

scale of the CB muons is at the 0.2% level

– J/psi Mass measured with SA muons shows a max 40 MeV discrepancy

Y

Page 12: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Local misalignmentStudying curvature offsets as a function of detector region

Page 13: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Effect of local misalignment

• Select Z samples with positive muon and Z sample with negative muon going into the problematic region

• Plot the quantity q(M(mm)-Mz)• Evident shift between the two distribution (about 1.5 GeV) • Due to the MS-ID Z misalignment (See next slides) • Both SA and ID measurement do not show this problem (CB only problem)

Page 14: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Assessing the magnitude of the effect

• Correct the effect in two ways:– Downweight the Z measurement in the MS

covariance matrix– Correct ZME and ThetaME for the measured

misalignment.

Page 15: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Option 1: Downweight Z ME

Bias greatly reduced proving that the effect is (mainly) given by the MS ID Z misalignment

Page 16: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Option 2: Correct for Z and Theta

Same result on Z mass

Will check if there are other local effects: ex:Study width of Z mass vs eta and phi

Page 17: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Effect of local misalignment and corrections

The correction has no effect on the overallmomentum scale and negligible effect on massresolution

Page 18: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Proposed systematics• Reprocessed the ZZ

candidates with the Z and Theta corrections

• One candidate moves by 1.7 GeV

• The average of the distribution (simple average no weighting) moves by less than 300 MeV

• Propose to use this method to assess the systematic error due to local misalignment.

Page 19: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Per event mass error• Work started:– Retrive momentum error per muon using standard MCP

resolution and smearing tool and propagate it in the Mass formula.

Page 20: MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.

Short term program

• Finalize absolute mass scale measurement with Z also as function of pt– Determine the systematic error to be assigned to the absolute

mass scale• Obtain coherency of results of J/PSI studies and between

J/Psi and Z studies in the low Pt regime• Continue checking for local misalignment other than the Z

and assess systematic error for the Z misalignment• Understand the per event error and the discrepancy on

the mass error obtained in the “ standard analysis” and the first results from the analysis using per event errors.