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Top Mass Template measurement in the Lepton Jets Channel PREBLESSING 1'7 fb1

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Jahred Adelman. University of Chicago. 7/26/07 TMT ... Fit a 2d parabola (including correlation cross-term) to the points. Example PE. 13. Jahred Adelman ... – PowerPoint PPT presentation

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Title: Top Mass Template measurement in the Lepton Jets Channel PREBLESSING 1'7 fb1


1
Top Mass Template measurement in the LeptonJets
ChannelPREBLESSING (1.7 fb-1)
2
Cast of characters
  • Jahred Adelman (UC)
  • Erik Brubaker (UC)
  • Sebastian Carron (Toronto)
  • Wojciech Fedorko (UC)
  • Young-Kee Kim (UC)
  • Hyun Su Lee (UC)
  • Young-Jang Lee (Seoul)
  • Mel Shochet (UC)
  • Pekka Sinervo (Toronto)
  • George Velev (FNAL)

Plus a (not completely all-volunteer) army of CAF
warriors
3
History and documentation
  • Published result Mtop 173.5 /- 3.9 GeV 355
    pb-1
  • PRL 96 022004 (2006)
  • PRD 73 032003 (2006)
  • Most recent preliminary result
  • Mtop 173.4 /- 2.8 GeV 680 pb-1
  • Recent CDF notes
  • CDF 8909 Lepton-Photon Mtop in ljets TMT2D
  • CDF 8824 Gen6 Pythia top-specific corrections
  • CDF 8761 Using KDE in Gen6 TMT
  • CDF 8190 KDE and its application to TMT
  • Soon well have a dilepton measurement too!
  • See Wojteks preblessing tomorrow
  • Web page
  • QA on out TWiki
  • http//www-cdf.fnal.gov/htbin/twiki/bin/view/TopMa
    ssTemplate/AnalysisLJ07

4
Reconstructing the top quark mass
  • Use standard LeptonJets ?2 fitter to reconstruct
    a single top quark mass (one number) per event
  • Correlated with true top quark mass, but not the
    same thing
  • Use overconstrained kinematics of ttbar system
  • New Pythia Gen6 TS corrections!

5
In-situ calibration using dijet mass
  • Kinematic fitter works well, but distributions
    are highly correlated not only to top quark mass,
    but also to JES
  • Introduce the dijet mass from the hadronically
    decaying W
  • Use as in situ calibration of JES
  • Strong JES correlation, also some weak top mass
    correlation
  • We use the dimass closest to the well-known W
    mass from any pair of untagged jets among leading
    4 jets (studied other choices, this was best)
  • New Throw away any events failing ?2 cut, just
    like for mtreco

6
Our likelihood
OLD
  • Likelihood simplified w.r.t. published analysis
  • Removed unwanted cross-terms
  • Event counting simpler, more correctx
  • Now mjj is a single number per event, so no
    correlations hidden there.
  • We want to account for correlations between
    mtreco and mjj, too!

NEW
7
Shape probability?
  • How do we get the probability to observe an event
    with mtreco and mjj?
  • Previously, assume the two observables are
    uncorrelated, and parameterize as a function of
    mtop and dJES
  • Near-impossible to account for correlation
    between observables
  • Parameterizations difficult, mathematically bad

New Use a Kernel Density Estimate-based approach
to form PDFs that are two-dimensional in
observables
8
A 1d KDE pictorial tutorial
Probability
Mtopreco
9
Types of KDE
Our nominal (2d) measurement
A cross-check (1dx1d) measurement
1Dx1D
Mtop RMS
2D
10
2d PDFs
11
Adaptive KDE
  • Want smoothing to depend on statistics within
    sample.
  • First pass Pilot density estimatesfixed kernel
    width.
  • Second pass Adaptive density estimates.
  • Narrower kernel in high-stats region ? sharper
    peak.
  • Wider kernel in low-stats region ? smoother tail.

12
How do we use this?
  • Have a grid of 2002 points in mass-JES space
    (mass 140-200, JES -3.0 to 3.0)
  • Minimize ns and nb for each subsample at every
    point in the grid
  • Fit a 2d parabola (including correlation
    cross-term) to the points

Example PE
13
Sample division
  • Old 1-tag(L) and 0-tag categories do not improve
    the expected total uncertainty at current
    luminosity
  • Increase systematics more than they reduce
    statistical error
  • After study, we require exactly four jets in
    1-tag category, but allow 3.5, 4, or more jets in
    2-tag

14
Boundary cuts
  • KDE doesnt know about hard cutoffs in the
    observables
  • Probability leaks into unpopulated regions
  • Easiest fix is to explicitly set boundaries and
    force kernels to stay inside.
  • Amounts to extra selection cut on mtreco, mjj
  • Efficiency high for signal events passing chi2 cut

15
Backgrounds (technical details)
  • Use MII4U numbers wonderfully provided by Tom
  • Use HFOR removal (jet-based)
  • Weight all the background samples by the
    individual pre-chi2 boundary efficiencies
    (50-80)
  • Use Alpgen weights to stitch together samples
  • Assume specific flavor backgrounds (ie Wbb) come
    from matrix element (ie btop?w samples)
  • Assume mistags come from Wlf (ie ptop?w samples)
  • Assume two-tag mistags are both mistags (not real
    tags)
  • Use event-by-event mistag probabilities
  • Assign QCD shape to mistags
  • Studied in previous incarnations, more
    cross-checks to come
  • Wbb/cc0-2P, Wc1-3P, W2-4P, s/t-stop, WW,
    WZ, ZZ
  • Events in PEs drawn according to their correct
    weight (including individual event mistag
    probabilities)

16
1dx1d Background PDFs
17
2d Background PDFs
18
Bias checks
JES gt 0 JES lt 0
  • No significant bias bias!
  • Slight JES bias (no matter)?
  • Pull width lt 1.0?!?!

19
On the pull width
  • Removing strange point at 168, pull width goes to
    98.1 and chi2/ndof becomes 5.3/6.0
  • Examined points at 168/log files/density
    estimates/PEs
  • Cannot find anything wrong with the point!
  • In any case, not reducing our reported error

Recall
20
Residual JES systematics
Systematics studied using large 175 GeV
sample Sum in quad of L1-L8 0.55 GeV/c2 Bkgd
JES uncertainty added linearly to uncertainty due
to first-order JES ( 0.38 GeV/c2 when converted
to a number in quadrature)
21
Other systematic samples
PEs 1.2 fb-1 run range vs PEs using 1.2 fb-1
ERR (in correct proportions). Take a systematic?
Or not?
22
Summary of systematics
  • Take MC uncertainty on sample for FSR (instead
    of 50 MeV)
  • PEs for b-jets and underway, should be done in
    next 1 day
  • No prescription yet for bkgd shape, taken from
    Gen5 Q2 variation on 1-tag and 2-tag samples
    only
  • Smaller now that we dont have 0-tag events!

23
Systematic vs Winter06 measurement
24
Nevt
25
The fit!
The fit!
26
Full fit
27
Cross-check 1dx1d fit
28
Are we lucky?
19.8
29
More cross-checks
n evt taken from minimization at single point
with best -ln(L), so not a full fit for number of
events (but a good approximation)
30
Cross-checks
31
Division by data period
No background constraint used (but JES constraint
used throughout)
32
2tag-1tag study
3.2 of PEs with observed num events have larger
2tag-1tag differences (8.0 for 2d sided
differences)
33
Fitted nbkgd
Paying no attention to strange spikes/dips
(stupid ROOT plotting issue), we prefer 0 2-tag
background in a wide area of the mass-JES plane
when bkgd constraint is removed
34
Old-style 1dx1d plots
35
Conclusions
  • Made a first measurement of the top quark mass in
    the LeptonJets Channel using gt 1 fb-1 of data
  • So far, single best top quark mass measurement
    from CDF
  • Machinery also being used to make a dilepton
    measurement (see Wojteks talk tomorrow!)
  • Measurements to be combined in future/for
    publication
  • Compare with previous TMT result using 680 pb-1
    Mtop 173.4 ? 2.3 GeV/c2

Mtop 171.6 ? 2.3 GeV/c2
36
Wait for it
Backups
37
Study of 2tag-only nobkgd corr PEs
38
Background composition
39
Anti-ele vs Wlf
KS prob (top group normalized PE version 77.5)
40
More adaptive KDE (signal)
41
More adaptive KDE (signal)
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