impact parameter resolution measurements from 900 gev lhc data

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Impact Parameter Resolution Measurements from 900 GeV LHC DATA Boris Mangano & Ryan Kelley (UCSD)

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Impact Parameter Resolution Measurements from 900 GeV LHC DATA. Boris Mangano & Ryan Kelley (UCSD). Outline. Samples and Event selection. Description of the method. Validation of the method on MC samples. - PowerPoint PPT Presentation

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Page 1: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

Impact Parameter Resolution Measurements

from 900 GeV LHC DATA

Boris Mangano & Ryan Kelley (UCSD)

Page 2: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.2

Outline

• Samples and Event selection.

• Description of the method.

• Validation of the method on MC samples.

• Measurement of Transverse and Longitudinal Impact Parameter resolutions on 900 GeV DATA.

Page 3: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.3

Samples and Event Selection

DATA:/MinimumBias/BeamCommissioning09-BSCNOBEAMHALO-Dec19thSkim_336p3_v1/RAW-RECO

MC:/MinBias/Summer09-STARTUP3X_V8K_900GeV-v1/GEN-SIM-RECO

Event Selection (see backup slides):

- BSC trigger and BH Veto (already applied at the level of the central skim)

- Tech.Trigger bit 0

- PhysicsDeclared bit

- NoScrapingEvent filter

- Only B=3.8 T runs

- Only E=900 GeV runs

Page 4: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.4

Preliminary RemarksDifferent Components affecting the IP measurement

Tk1 is from decay-in-flight. Its d01, wrt the Primary Vertex, is genuinely ≠0.

Tk2 is a prompt track. Its d02 is exactly = 0.

Tk1

Tk2

d01 PV

Case 1) Exactly known trajectories and perfectly known collision point (SimTracks and SimVertex)

Case 2) Exactly known trajectories, but measured collision point (SimTracks and reco PV)

Both Tk1 and Tk2 have d0 different from their true values because of the “smearing” due to the vertex position resolution

d0 = d0true “vertex smearing”

Tk1

Tk2

true PV

reco PV

Page 5: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.5

Preliminary RemarksDifferent Components affecting the IP measurement

Case 3) Both trajectories and collision point are not exactly know because they are both measured

=

Real World

Both Tk1 and Tk2 have d0 different from their true values because of the “smearing” due to the vertex position resolution and the smearing due to the finite resolution on the track parameters

d0meas = d0true “vertex smearing” “track impact parameter resolution”

Tk1

Tk2

reco PV

reco Tk1

reco Tk2

Page 6: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.6

Preliminary RemarksDifferent Components affecting the IP measurement

d0meas = d0true “vertex smearing” “track impact parameter resolution”

The agreement between the resolutions of the primary vertex position measurements in DATA and MC has already been proved by Y.Gao, F.Fiori et al.

https://twiki.cern.ch/twiki/bin/view/CMS/PrimaryVertexResolution

In the rest of the talk, focusing on the effect of vertex resolution on the IP measurement: “vertex smearing”

Final observable measured by this analysis

Page 7: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.7

Description of the method

1) Select only events with the primary vertex fitted from 10-16 tracks (see next).

2) For a given track with measurements on 8 Tracker layer (2 pixels), refit the

primary vertex using all the other tracks in the event.

3) For the same track, evaluate d0 and dz w.r.t. the refitted vertex position.

4) Repeat 2-3 for all the other tracks in the event that pass the selection.

5) Save the previously evaluated d0 and dz values in bins of track’s pT and eta.

7) Repeat 2-5 for all the selected events.

Page 8: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.8

Description of the method (II)8) Fit each pT and eta bin using the function

F = VertexSmearingFunction IP ResolutionFunction

Measured d0 wrt recoPV [m] Vertex “smearing” pdf [m] Impact parameter resolution [m]

Measured from data Estimated from MC Extracted from the Fit of the convolution function F

Page 9: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.9

The d0 and dz calculated in this way were put in separate histograms for distinct SimTrack’s pT and eta values.

Vertex “smearing” pdf [m]

--- narrower gaussian

--- wider gaussian

--- 2 gaussian sum = VertexSmearing pdf

--- narrower gaussian

--- wider gaussian

--- 2 gaussian sum = VertexSmearing pdf

The d0 and dz of simulated SimTracks were evaluated with respect to the reconstructed PV position on the MC sample.

Each bin is fitted by a 2-gaussian sum function.

Tk1

Tk2

true PV

reco PV

Evaluation of the VertexSmearing function

Page 10: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.10

Evaluation of the VertexSmearing function

Ve

rte

x s

me

ari

ng

pd

f

[m

]V

ert

ex

sm

ea

rin

g p

df

[m

] Vertex smearing for d0 as a function of the track’s pT

Vertex smearing for d0 as a function of the track’s eta

Vertex smearing for dz as a function of the track’s eta

Track’s pT [GeV/c]

Track’s pT [GeV/c] Track’s eta

Track’s eta

Vertex smearing for dz as a function of the track’s pT

Page 11: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.11

Evaluation of the Impact Parameter Resolution

Data are fit using the convolution function F, where only the parameters of the “IP ResolutionFunction” (a single gaussian) are unconstraint.

Measured d0 wrt recoPV [m]Vertex “smearing” pdf [m]

F = VertexSmearingFunction IP ResolutionFunction

The use of a single gaussian for modeling the resolution function is appropriate if:

- The pT and eta of the tracks contributing to the same histogram are sufficiently “close”.

- Only the core of the distribution is considered (2sigma fit)

Page 12: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.12

Validation of the method on MCTransverse Impact Parameter Resolution

Additional Track cut:

|eta| < 0.4

Additional Track cut:

|eta| < 0.4

Good agreement between the “measured” resolutions (red) and the mc-truth-determined resolutions (black).

Good agreement between the “measured” resolutions (red) and the mc-truth-determined resolutions (black).

Page 13: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.13

Track selection:

0.75 < |pT| < 0.85 (GeV)

Track selection:

0.75 < |pT| < 0.85 (GeV)

Track selection:

1.0 < |pT| < 1.4 (GeV)

Track selection:

1.0 < |pT| < 1.4 (GeV)

Validation of the method on MCTransverse Impact Parameter Resolution

Page 14: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.14

Track selection:

0.75 < |pT| < 0.85 (GeV)

Track selection:

0.75 < |pT| < 0.85 (GeV)

Track selection:

1.0 < |pT| < 1.4 (GeV)

Track selection:

1.0 < |pT| < 1.4 (GeV)

Validation of the method on MCLongitudinal Impact Parameter Resolution

Page 15: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.15

Results from 900 GeV DATA

Track cut:

|eta| < 0.4

Track cut:

|eta| < 0.4

Page 16: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.16

Results from 900 GeV DATA

Track selection:

0.75 < |pT| < 0.85 (GeV)

Track selection:

0.75 < |pT| < 0.85 (GeV)

Track selection:

1.0 < |pT| < 1.4 (GeV)

Track selection:

1.0 < |pT| < 1.4 (GeV)

Page 17: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.17

Results from 900 GeV DATA

Track cut:

|eta| < 0.4

Track cut:

|eta| < 0.4

Page 18: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.18

Results from 900 GeV DATA

Track selection:

0.75 < |pT| < 0.85 (GeV)

Track selection:

0.75 < |pT| < 0.85 (GeV)

Track selection:

1.0 < |pT| < 1.4 (GeV)

Track selection:

1.0 < |pT| < 1.4 (GeV)

Page 19: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.19

ConclusionsMethod to estimate the Track Impact Parameter Resolution from DATA has been implemented and described in this talk.

The Method has been successfully validated on MC and used on 900 GeV DATA from December 2009 runs.

Results based on 900 GeV DATA are very close to values expected from STARTUP MC. Impact Parameter resolutions are just slightly worse.

Overall, the analysis will benefit from higher LHC energy events for which there are more high pT tracks from the collision and the uncertainty on the primary vertex position is smaller.

TWIKI page and Analysis Note in preparation: https://twiki.cern.ch/twiki/bin/viewauth/CMS/ImpactParameterResolutionDec2009

Page 20: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.20

BACKUP SLIDES

Page 21: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.21

Event Selection for DATA (and that you don’t usually apply on a MC sample)

1) Require Tech.Trigger bit 0 (i.e. BPTX coincidence): it selects events in beam-beam bunch crossings. Discards single-beam BXs and empty BXs.

2) Require Tech.Trigger bit 40 or 41 (i.e. BSC triggers): selects events with activity compatible with a collision

3) Veto on Tech.Trigger bit 36-39 (BeamHalo triggers)

Page 22: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.22

Event Selection for DATA (II)(and that you don’t usually apply on a MC sample)

4) Discard events for which B!=3.8, e.g. events collected during the magnet ramping to its nominal value.

4’) For this study only, discard events from 2.36 TeV runs

Discarded runs: 123967-123997, 124119,124120,124275

5) Require PhysicsDeclared bit: this bit is set to TRUE when all the CMS components are declared OK for data taking: e.g. all the HighVoltages of the Tracker sensors are ON.

Page 23: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.23

Event Selection for DATA (III) (and that you don’t usually apply on a MC sample)

6) Reject beam-background events (AKA pixel monster events, AKA scraping event).

The NoScraping event filter has been used: it requires >25% of tracks in the event to be “highPurity” tracks.

Page 24: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.24

Track selection:

|eta| < 0.4

Track selection:

|eta| < 0.4

Validation of the method on MCLongitudinal Impact Parameter Resolution

Some bins looks problematic

Page 25: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.25

Validation of the method on MCLongitudinal Impact Parameter Resolution

After smoothing of the response function, the final fit is more stable

There are less “problematic” bins

Page 26: Impact Parameter Resolution Measurements  from 900 GeV LHC DATA

B.ManganoBTV POG meeting - 29/3/2010 Pag.26

Effect of the resolution on the Primary Vertex position

1) Are the reconstructed primary vertices of the MC (used to estimate the response function) consistent with DATA?

From Y.Gao:

https://twiki.cern.ch/twiki/bin/view/CMS/PrimaryVertexResolution

2) Anyway, how much the Impact Parameter Resolution measurement is sensitive to the vertex smearing? See next slides..