VELO systematics and physics LHCb VELO meeting, CERN, 28 March 2008

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Presentation transcript:

VELO systematics and physics LHCb VELO meeting, CERN, 28 March 2008 Eduardo Rodrigues University of Glasgow LHCb VELO meeting, CERN, 28 March 2008

VELO systematics and physics What are VELO systematics? Any systematic effects / biases introduced by mis-understanding / simplifications of VELO calibration / response / data reconstruction / … General thoughts VELO group has so far focused on detector design, construction, installation and commissioning Time to use all the expertise to bridge with studies of relevance to physics analysis Group needs to tackle assessment/impact of VELO performance on the quality of the physics output We are in an ideal situation to do so … ;-) Eduardo Rodrigues

A non-exhaustive shopping list Main idea: Brainstorming with VELO experts on areas of reconstruction that can be improved among those that have most impact on physics performance Improvements in clustering algorithms Eta correction to cluster position  impact on tracking? Tuning of resolutions with data: so far simulation has tuning from test-beam data, but better estimate resolutions directly from data Cross-talk corrections from data: is this issue fully solved? Do we have the machinery in place and implemented? Study of calibration strategies from (real) data VELO data quality and vertexing (measurements errors) B-field in VELO: really negligible / irrelevant for e.g. Ks analyses? Propertime resolution models studies: c.f. studies from Laurence Carson, see next page Some of these issues are also relevant for the trigger Effects of VELO misalignments on quality of physics analyses  discussed here, today … Eduardo Rodrigues

Propertime resolution model for Bhh Laurence Carson, Glasgow The proper time is defined as The proper time resolution, στ , of the detector needs to be known because it dilutes ACP: Goal: Determine resolution model directly from data Using propertime value and error on an event-by-event basis Studies near completion Laurence will present full details soon at propertime WG … stay tuned! Eduardo Rodrigues

Impact of VELO misalignments on physics Work done with Marco Gersabeck and Jacopo Nardulli (Full account given at the Tracking and Alignment Workshop in Ferrara, 28 Feb. 2008)

Analysis of the B  hh decay channel Outline Specific case studied Analysis of the B  hh decay channel Motivation and overview Implementation of misalignments - misalignment scales and conditions databases - data samples Impact of misalignments on selection of B  hh decays - pattern recognition and reconstruction performance - selection variables Impact of misalignments on combined B  hh fit - RooFit analysis of combined B  hh decays Eduardo Rodrigues

Motivation and overview Systematic study of effect of misalignments purely based on their size Does not involve any assumptions on quality of metrology or alignment software Gives a good overview and shows critical alignment degrees-of-freedom Effects on selection and subsequent CP-sensitivity analysis We also plan to study remaining misalignment effects after application of alignment algorithms Identify potential problems/biases of alignment procedure Eduardo Rodrigues

Implementation of misalignments Eduardo Rodrigues

Procedure (1/2) Misaligned databases: Create random misalignments for VELO sensors/modules Choose scale (Gaussian sigma) to be ~1/3 of the detector single hit resolution (called “1s”) Generate 10 sets of “1s” misalignments Likewise, create similar sets with misalignment scales increased by factors of 3 (3s) and 5 (5s) Every 10 sets of VELO 1s / 3s / 5s misalignments stored in a conditions database  3 (small) slice databases in total: - VELO 1s / 3s / 5s misalignments Eduardo Rodrigues

Procedure (2/2) Data samples: Event processing: Generate 10 x 2k events each of which with a different set of the 10 sets of “1s” misalignments  20k B  pp events for each of the misalignment scenarios: no misalignment (0s) 1s / 3s / 5s misalignments for VELO suppressing potentially “friendly” or “catastrophic” misalignment sets In total, 80k B  pp events generated Event processing: Events generated with perfect geometry (up to DIGI level) DSTs produced with Brunel version v32r2, misalignments applied solely at reconstruction level Physics analysis later performed with DaVinci v19r9 Eduardo Rodrigues

Misalignment scales and conditions databases Scales for the “1s” misalignment set: SUB-DETECTOR Translations (mm) Rotations (mrad) Dx Dy Dz Rx Ry Rz VELO sensor 3 10 1.00 0.20 VELO module Eduardo Rodrigues

Impact of misalignments on selection of B  hh decays Eduardo Rodrigues

The B  hh analysis, in short (1/2) Goal: Extraction of g angle from B  pp and Bs  KK events From measurement of CP asymmetries assuming U-spin symmetry Sensitivity to CP parameters such as Im(lf) and Re(lf) and Dms, DGs, wtag  g, d and q can be determined once C and S are known (U-spin symmetry at 20% level) Hadronic parameters d and q parameterize magnitude and phase of penguin-to-tree amplitude ratio Analysis involves several B  hh’ decays, where h = p, K Eduardo Rodrigues

The B  hh analysis, in short (2/2) Selection cuts consist of various requirements: Particle identification: K-p separation based on PID likelihood difference (DlnLKp) Topological: clear separation of primary vertex and B-decay vertex B-daughters impact parameter (IP) and B-decay length significance Kinematic: minimal B-candidate and B-daughters transverse momentum Vertexing: c2 of vertex fit to B-daughters Mass: mass window cut on invariant mass of B-daughters Eduardo Rodrigues

Impact of VELO misalignments (1/10) Selected event numbers and pattern recognition efficiencies after standard B  hh selection Nselected B ePatForward (%) eMatching (%) 0s 4229 85.9 81.1 1s 3904 85.6 80.9 3s 2241 83.1 78.3 5s 1106 80.1 75.5 Effect on pattern recognition is small-ish Very significant loss of events, has to come from the selection itself …  misalignments have serious impact on some selection variables  systematic check of all of them … Eduardo Rodrigues

Impact of VELO misalignments (2/10) Example of PR efficiency distributions obtained with the 10 sets of 2k events produced with Brunel VELO 5s no misalignment VELO 5s Eduardo Rodrigues

Impact of VELO misalignments (3/10) ------------------------------------- Pat. Rec. : # tracks Ghost rate VeloRZ : 87 10.41 % Velo3D : 79 7.02 % VeloTT : 10 25.44 % Forward : 30 15.36 % Match : 27 11.28 % TSA : 56 9.68 % Downstream : 35 36.66 % Best : 109 21.06 % ------------------------------------- Pat. Rec. : # tracks Ghost rate VeloRZ : 88 10.44 % Velo3D : 79 7.32 % VeloTT : 10 25.61 % Forward : 30 15.47 % Match : 27 11.35 % TSA : 56 9.68 % Downstream : 35 36.66 % Best : 109 21.28 % 0s 1s ------------------------------------- Pat. Rec. : # tracks Ghost rate VeloRZ : 88 10.56 % Velo3D : 76 9.81 % VeloTT : 10 28.13 % Forward : 30 16.67 % Match : 26 12.46 % TSA : 56 9.68 % Downstream : 35 36.66 % Best : 107 23.13 % ------------------------------------- Pat. Rec. : # tracks Ghost rate VeloRZ : 88 10.96 % Velo3D : 73 12.54 % VeloTT : 9 30.63 % Forward : 29 18.03 % Match : 26 13.82 % TSA : 56 9.68 % Downstream : 35 36.66 % Best : 104 25.13 % 3s 5s Eduardo Rodrigues

Impact of VELO misalignments (4/10) -------------------------------------------------------------- Pat. Rec. : Efficiency Clones long long > 5 GeV long long > 5 GeV VeloRZ : 98.0 % 98.9 % 2.4 % 1.8 % Velo3D : 97.0 % 98.2 % 2.4 % 1.9 % VeloTT : 2.4 % 1.0 % 1.1 % 0.8 % Forward : 85.9 % 93.1 % 1.8 % 1.4 % Match : 81.1 % 88.2 % 0.0 % 0.0 % TSA : 91.8 % 95.9 % 0.7 % 1.0 % Best : 97.4 % 98.6 % 5.2 % 3.3 % 0s -------------------------------------------------------------- Pat. Rec. : Efficiency Clones long long > 5 GeV long long > 5 GeV VeloRZ : 98.0 % 98.9 % 2.4 % 1.8 % Velo3D : 96.7 % 98.0 % 2.5 % 1.9 % VeloTT : 2.4 % 0.9 % 1.1 % 1.0 % Forward : 85.6 % 92.9 % 1.8 % 1.4 % Match : 80.9 % 88.0 % 0.0 % 0.0 % TSA : 91.8 % 95.9 % 0.7 % 1.0 % Best : 97.3 % 98.5 % 5.2 % 3.4 % 1s Eduardo Rodrigues

Impact of VELO misalignments (5/10) -------------------------------------------------------------- Pat. Rec. : Efficiency Clones long long > 5 GeV long long > 5 GeV VeloRZ : 98.0 % 98.8 % 2.8 % 2.2 % Velo3D : 93.9 % 96.2 % 2.9 % 2.3 % VeloTT : 2.2 % 0.9 % 1.5 % 1.1 % Forward : 83.1 % 90.8 % 2.1 % 1.7 % Match : 78.3 % 85.9 % 0.0 % 0.0 % TSA : 91.8 % 95.9 % 0.7 % 1.0 % Best : 96.2 % 98.0 % 5.7 % 3.9 % 3s -------------------------------------------------------------- Pat. Rec. : Efficiency Clones long long > 5 GeV long long > 5 GeV VeloRZ : 97.7 % 98.4 % 3.8 % 3.5 % Velo3D : 91.1 % 94.1 % 3.4 % 2.8 % VeloTT : 2.1 % 0.9 % 1.9 % 1.1 % Forward : 80.1 % 88.2 % 2.4 % 1.9 % Match : 75.5 % 83.4 % 0.0 % 0.0 % TSA : 91.8 % 95.9 % 0.7 % 1.0 % Best : 95.1 % 97.2 % 6.2 % 4.5 % 5s Eduardo Rodrigues

Impact of VELO misalignments (6/10) -------------------------------------------------------------- Pat. Rec. : Purity Hit efficiency long long > 5 GeV long long > 5 GeV VeloRZ : 99.5 % 99.6 % 96.5 % 97.4 % Velo3D : 99.3 % 99.4 % 95.7 % 97.1 % VeloTT : 98.4 % 98.0 % 93.2 % 93.8 % Forward : 98.8 % 99.0 % 94.8 % 96.9 % Match : 99.2 % 99.3 % 87.3 % 87.8 % TSA : 98.3 % 98.3 % 87.9 % 88.4 % Best : 98.7 % 98.9 % 89.6 % 94.1 % 0s -------------------------------------------------------------- Pat. Rec. : Purity Hit efficiency long long > 5 GeV long long > 5 GeV VeloRZ : 99.5 % 99.6 % 96.5 % 97.4 % Velo3D : 99.3 % 99.4 % 95.4 % 96.9 % VeloTT : 98.4 % 98.0 % 92.8 % 93.4 % Forward : 98.8 % 98.9 % 94.8 % 96.9 % Match : 99.2 % 99.3 % 87.3 % 87.8 % TSA : 98.3 % 98.3 % 87.9 % 88.4 % Best : 98.7 % 98.8 % 89.5 % 93.9 % 1s Eduardo Rodrigues

Impact of VELO misalignments (7/10) -------------------------------------------------------------- Pat. Rec. : Purity Hit efficiency long long > 5 GeV long long > 5 GeV VeloRZ : 99.5 % 99.6 % 96.2 % 97.0 % Velo3D : 98.9 % 99.0 % 93.0 % 95.0 % VeloTT : 97.9 % 97.3 % 90.0 % 90.8 % Forward : 98.7 % 98.9 % 94.8 % 96.9 % Match : 99.1 % 99.2 % 87.4 % 87.8 % TSA : 98.3 % 98.3 % 87.9 % 88.4 % Best : 98.5 % 98.7 % 88.0 % 92.5 % 3s -------------------------------------------------------------- Pat. Rec. : Purity Hit efficiency long long > 5 GeV long long > 5 GeV VeloRZ : 99.5 % 99.5 % 95.0 % 95.7 % Velo3D : 98.4 % 98.6 % 90.0 % 92.2 % VeloTT : 97.3 % 96.3 % 86.8 % 86.5 % Forward : 98.6 % 98.8 % 94.8 % 96.8 % Match : 99.0 % 99.1 % 87.4 % 87.8 % TSA : 98.3 % 98.3 % 87.9 % 88.4 % Best : 98.2 % 98.4 % 86.1 % 90.5 % 5s Eduardo Rodrigues

Impact of VELO misalignments (8/10) Integrating … Biggest effect comes from tight upper cut on the B-candidate IP significance, IPS < 2.5 Additional effect on lower IPS cut of B-daughters Also c2 of B-vertex fit is rather affected Eduardo Rodrigues

Impact of VELO misalignments (9/10) Propertime resolution after standard B  hh selection t resolution (fs) 0s 37.7 1s 39.4 3s 58.1 5s 82.0 0s 1s 3s 5s (sigma of Gaussian fit) 2nd order effects: B-daughters momentum resolution: 0.50  0.52 % B mass resolution: 22.5  23.5 MeV Eduardo Rodrigues

First ever check of impact of misalignments on vertex resolutions Impact of VELO misalignments (10/10) Primary vertex and B-decay vertex resolutions in selected B  hh events Resolution Primary vertex (mm) x/y z B-decay vertex (mm) 0s 9 41 14 147 1s 10 48 15 155 3s 16 81 21 226 5s 25 29 262 First ever check of impact of misalignments on vertex resolutions Eduardo Rodrigues

Impact of combined VELO, IT and OT misalignments One can do the same kind of analysis for misalignments of the other tracking stations Full account given at the Tracking and Alignment Workshop in Ferrara, 28 Feb. 2008 RESOLUTION Affected by VELO misalignments T misalignments B-daughters momentum no yes B mass B vertex B Impact Parameter B propertime Eduardo Rodrigues (“no” taken here as “small effect”)

Impact of misalignments on combined B  hh fit Eduardo Rodrigues

The B2hhFit toy MC fitter, in short Allows for CP-sensitivity studies with B  hh decays Fast toy Monte Carlo fitter “” based on RooFit to study effect of misalignments purely based on their size Combined fit of 8 B/B  hh’ decays An unbinned extended maximum likelihood fit is performed on the combined conditional PDF of the mass and time signal and background events (with >17 free parameters) Uses as input outcome of B  hh selection studies such as propertime and mass resolutions I will not present many details here (see Ferrara presentation) Just examples to get a feeling … Work ongoing … (Typical output: invariant mass distribution) Eduardo Rodrigues

Typical B2hhFit toy results (1/2) Checked effect of mass resolution: 22.5  25.5 (VELO & IT/OT 5s misalignments)  30.0 MeV (“extreme case”) 22.5 MeV 30.0 MeV Errors on fitted parameters tend to increase, but only marginally Pull distributions do not deteriorate, i.e. fit quality does not “collapse” Though biases in pulls increase slightly Eduardo Rodrigues

Typical B2hhFit toy results (2/2) Example of Bs fit Checked effect of propertime resolution: 0s 5s 0s 5s Eduardo Rodrigues

VELO alignment results on testbeam data Outlook and future Impact of VELO misalignments has been assessed in detail “throughout the analysis chain” - VELO misalignments strongly affect selection and propertime and IP resolutions If software alignment is of order or better than “1sigma” we are in business! (effect of z-scaling presently being investigated …) We should encourage further work on impact of “VELO systematics” on physics! x,y 0.9μm VELO alignment results on testbeam data z 2μm Eduardo Rodrigues