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Detector simulations for EIC at BNL Alexander Kiselev POETIC Workshop Sep,2-5 2013.

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Presentation on theme: "Detector simulations for EIC at BNL Alexander Kiselev POETIC Workshop Sep,2-5 2013."— Presentation transcript:

1 Detector simulations for EIC at BNL Alexander Kiselev POETIC Workshop Sep,2-5 2013

2 Sep,3 2013A.Kiselev Contents  Dedicated eRHIC detector concept  EicRoot framework  General idea  Tracking studies  Calorimeter R&D  Tools for detector development  EIC detector solenoid field modeling  Update on EIC smearing generator  Summary

3 eRHIC detector concept Sep,3 2013A.Kiselev

4  =10.03 mrad 1.512 m 5.475 m IPIP 4.50 m  =10 mrad.9 cm (p o /2.5) ZDCZDC  =10 mrad  =6.2 mrad 1.53m 0.81 m 1.95 m 0.993 m neutrons Ion beam 2 4 6 8 1212 1414 1616 1010 0.83m 0.1678 m 0.1733 m 0. 3 2 m x y z Electron quadrupoles Combined function magnet Quad 3 Quad 2 Dipole 4.50 m Solenoid aligned with ion beam INSIDE OUTSIDE ions electrons 2.5 m Interaction Region design Sep,3 2013A.Kiselev

5 0.44843 m Q5 D5 Q4 90.08703 m 60.0559 m 10 3 m 4.5  =4 mrad 8.18 m  =9.82 mrad 10 mrad 5.475 m 30 20 40 50 15.1 m 0.316 m  =3.6745 mrad Interaction Region design Sep,3 2013A.Kiselev

6 Sep,3 2013A.Kiselev eRHIC detector layout (E e ~ 20 GeV)

7 Sep,3 2013A.Kiselev eRHIC detector layout (E e < 10 GeV)

8 Sep,3 2013A.Kiselev eRHIC detector view (August’2013) EMC and tracking detectors ~implemented so far Central EMC Backward EMC Forward EMC SOLENOID RICH

9 EicRoot framework Sep,3 2013A.Kiselev

10 Sep,3 2013A.Kiselev EIC detector in FairRoot framework  FairRoot is officially maintained by GSI  O(10) active experiments  O(100) users Interface to GEANT Interface to ROOT event display Parameter database MC stack handling … EicRoot PandaRootFopiRoot FairBase Interface to FairBase classes Ideal track finder Interface to GenFit … TPC digitization Real life track finder(s) Another GenFit interface Interface to RAVE eic-smear Generator output file import Fast smearing codes solenoid modeling

11 Sep,3 2013A.Kiselev End user view -> MC points simulation No executable (steering through ROOT macro scripts) digitization“PID” Passreconstruction -> Hits-> “Short” tracks -> Clusters -> “Combined” tracks -> Vertices @ IP ROOT files for analysis available after each step C++ class structure is well defined at each I/O stage

12 Tracking studies Sep,3 2013A.Kiselev

13 Sep,3 2013A.Kiselev Requirements for EIC main tracker As low material budget as possible Complete geometric coverage in the  range [-3.. 3] Momentum resolution not worse than ~3%, even at large rapidities

14 Sep,3 2013A.Kiselev Tracking code implementation Magnetic field interface exists Detector geometry is described in 0-th approximation: Digitization exists (simplistic, except for TPC where FopiRoot codes allow to perform a complete digi chain) “Ideal” track reconstruction inherited from PandaRoot codes Real-life track finding&fitting as well as vertex finding&fitting inherited from FopiRoot codes (work in progress) Silicon vertex tracker Silicon forward/backward tracker TPC GEM forward/backward tracker MRS-B1 solenoid design per default

15 Sep,3 2013A.Kiselev Vertex silicon tracker MAPS technology; ~20x20mm 2 chips, ~20  m 2D pixels STAR detector upgrade “building blocks” (cable assemblies)

16 Sep,3 2013A.Kiselev Vertex silicon tracker 6 layers at [30..160] mm radius 0.37% X 0 in acceptance per layer simulated precisely digitization: single discrete pixels, one-to-one from MC points

17 Sep,3 2013A.Kiselev Other tracking elements 2x7 disks with up to 180 mm radius N sectors per disk; 200  m silicon-equivalent thickness digitization: discrete ~20x20  m 2 pixels forward/backward silicon trackers: TPC: GEM trackers: ~2m long; gas volume radius [200..800] mm 1.2% X 0 IFC, 4.0% X 0 OFC; 15.0% X 0 aluminum end-caps digitization: 1) idealized, assume 1x5 mm GEM pads; 2) complete (FopiRoot source codes adapted, GEM pad shape tuning in progress) 3 disks behind the TPC end-caps STAR FGT design digitization: 100  m resolution in X&Y; gaussian smearing

18 Sep,3 2013A.Kiselev EIC tracker view (August’2013) Backward GEM Tracker Backward Silicon Tracker TPC Vertex Silicon Tracker Forward GEM Tracker Forward Silicon Tracker

19 Sep,3 2013A.Kiselev Example plots from tracking code 1 GeV/c   tracks at  32 GeV/c   tracks at  = 206 = 9 -> look very reasonable from statistical point of view

20 Sep,3 2013A.Kiselev Momentum resolution plot #1   track momentum resolution vs. pseudo-rapidity -> expect 2-3% or better momentum resolution in the whole kinematic range

21 Sep,3 2013A.Kiselev Momentum resolution plot #2   track momentum resolution at  vs. Silicon thickness -> ~flat over inspected momentum range because of very small Si pixel size

22 Sep,3 2013A.Kiselev Momentum resolution plot #3 p + track momentum resolution at h = 3.0 vs. Silicon pixel size -> 20 micron pixel size is essential to maintain good momentum resolution

23 EIC solenoid modeling Sep,3 2013A.Kiselev

24 Sep,3 2013A.Kiselev EIC solenoid modeling Yield large enough bending for charged tracks at large  Keep field inside TPC volume as homogeneous as possible Keep magnetic field inside RICH volume(s) small main requirements: Presently used design: MRS-B1 -> use OPERA-3D/2D software

25 Sep,3 2013A.Kiselev EIC solenoid modeling Other options investigated, like 4-th concept solenoid design -> obviously helps to cancel “tails”

26 EIC smearing generator Sep,3 2013A.Kiselev

27 Sep,3 2013A.Kiselev General architectureSmearer: Performs fast detector smearing MC generator output MC tree code: Builds ROOT tree containing events eic-smear C++ code running in ROOT Builds with configure/Make Single libeicsmear.so to load in ROOT gmc_tran s Milou Rapga p PEPSI DPMjet Django h PYTHI A

28 Sep,3 2013A.Kiselev Functionality built in Function defining σ(X) = f([E, p, θ, φ]) (single) quantity, X, to smear: E, p, θ, φ ++ Acceptance for X in E, p, θ, φ, pT, pZ Easily configurable acceptance definitions Kinematic variable smearing declarations either a priori knowledge of detector resolutions is needed or parameterization based on a full GEANT simulation -> try out resolutions provided by EicRoot fits …

29 Sep,3 2013A.Kiselev Hadron identification with RICH -> pion/kaon/proton separation must be possible up to momenta ~40 GeV/c consider hadrons in pseudo-rapidity range ~[1.0.. 3.0]

30 Sep,3 2013A.Kiselev Migration in (x,Q 2 ) bins 10GeV x 100GeV beams -> “survival probability” is above ~80% in the region where tracking has superior resolution compared to calorimetry

31 Sep,3 2013A.Kiselev EicRoot Interface to eic-smear  EicRoot input  EicRoot output directly uses eic-smear library calls to import ASCII event files after MC generators … … as well as “unified” ROOT format event files is available in eic-smear format with charged particle momentum variables “smeared” by Kalman Filter fit after track reconstruction … … while other variables modified by smearing generator according to its recipes

32 Calorimeter R&D Sep,3 2013A.Kiselev

33 Sep,3 2013A.Kiselev EM calorimeter requirements Complete geometric coverage in the  range [-4.. 4] Very good (~1-2 %/√E) backward end-cap (electron going direction) resolution Moderate (~10-12 %/√E) resolution for forward and central parts High granularity (angular resolution better than 1 o ) Compactness of barrel calorimeter

34 Sep,3 2013A.Kiselev Calorimeter code implementation Written from scratch Unified interface (geometry definition, digitization, clustering) for all EIC calorimeter types Rather detailed digitization: configurable light yield exponential decay time; light collection in a time window attenuation length; possible light reflection on one “cell” end SiPM dark counting rate; APD gain, ENF, ENC configurable thresholds

35 Sep,3 2013A.Kiselev Backward EM Calorimeter (BEMC) PWO-II, layout a la CMS & PANDA (but no cooling) -2500mm from the IP both projective and non-projective geometry implemented digitization based on parameters taken from PANDA R&D 10 GeV/c electron hitting one of the four BEMC quadrants Same event (details of shower development)

36 Sep,3 2013A.Kiselev BEMC energy resolution plot #1 -> projective geometry may lag behind in terms of resolution? electrons at 

37 Sep,3 2013A.Kiselev BEMC energy resolution plot #2 “Realistic” digitization stands for: light yield 17pe/MeV; APD gain 50, ENF 2.0, ENC 4.2k; 10 MeV single cell threshold; non-projective geometry; 

38 Sep,3 2013A.Kiselev Forward EM Calorimeter (FEMC) STAR e/m calorimeter upgrade building blocks (tungsten powder scintillating fiber sampling technology) 1mm fibers; sampling fraction for e/m showers ~2.6% +2500mm from the IP; non-projective geometry “medium speed” simulation (up to energy deposit in fibers) reasonably detailed digitization; “ideal” clustering code

39 Sep,3 2013A.Kiselev FEMC energy resolution study -> good agreement with original MC studies and measured data “Realistic” digitization stands for: 40MHz SiPM noise in 50ns gate; 4m attenuation length; 5 pixel single tower threshold; 70% light reflection on upstream fiber end; 3 degree track-to-tower-axis incident angle

40 Sep,3 2013A.Kiselev FEMC tower “optimization” original mesh optimized mesh -> optimized mesh design can probably decrease “constant term” in energy resolution

41 Sep,3 2013A.Kiselev Central EM Calorimeter (CEMC) same tungsten powder + fibers technology as FEMC, … … but towers are tapered non-projective geometry; radial distance from beam line [815.. 980]mm -> barrel (central) calorimeter collects less light, but response (at a fixed 3 o angle) is perfectly linear

42 Sep,3 2013A.Kiselev CEMC energy resolution plot #1 -> simulation does not show any noticeable difference in energy resolution between straight and tapered tower calorimeters 3 degree track-to-tower-axis incident angle

43 Sep,3 2013A.Kiselev CEMC energy resolution plot #2 -> energy response goes down with polar angle because of effectively decreasing sampling fraction; quite reasonable 8 GeV/c electrons

44 EicRoot as a tool for detector development Sep,3 2013A.Kiselev

45 Sep,3 2013A.Kiselev EicRoot availability SVN -> http://svn.racf.bnl.gov/svn/eic/eicroothttp://svn.racf.bnl.gov/svn/eic/eicroot eic000* cluster -> /eic/data/FairRoot README & installation hints Few basic usage examples

46 Sep,3 2013A.Kiselev Tracker “designer” tools  Allow, among other things  to add “simple” tracking detector templates to the “official” geometry  to try out various magnetic field maps  Require next to zero coding effort -> see tutorials/designer/tracking directory for details Which momentum resolution for 10 GeV/c pions will I get with 10 MAPS layers at 

47 Sep,3 2013A.Kiselev Tracker “designer” tools Create geometry file (few dozens of lines ROOT C script) Include few lines in “standard” sim/digi/reco scripts: Analyze output ROOT file -> workflow sequence:

48 Sep,3 2013A.Kiselev Calorimeter “designer” tools  Allow to easily add “simple” calorimeter detector templates to the “official” geometry  Require next to zero coding effort Which energy resolution for 1 GeV/c electrons will I get with a “basic” PWO calorimeter 

49 Sep,3 2013A.Kiselev Calorimeter “designer” tools  As long as the following is true:  … one can with a moderate effort (99% of which is writing a ROOT C macro with geometry and mapping description) build custom EicRoot-friendly calorimeter which can be used for both standalone resolution studies and/or as an optional EIC device (and internal cell structure does not matter) -> see tutorials/designer/calorimetry directory for details your dream calorimeter is a logical 2D matrix … … composed of “long cells” as elementary units, all the game is based on (known) light output per energy deposit, energy resolution after “ideal” digitization suffices as a result

50 Calorimeter R&D Sep,3 2013A.Kiselev (by-product for PHENIX upgrade)

51 PHENIX upgrade calorimeter setup Sep,3 2013A.Kiselev tungsten scintillating fiber epoxy sandwich default configuration: 1mm fibers; 7 fiber layers per 20x20 mm 2 “tower” sampling fraction for e/m showers ~2.3% 10 cm Pure tungsten metal sheet (  ~ 19.3 g/cm 3 ) Thickness ~ 0.5-1.0 mm Tungsten powder epoxy (  ~ 10-11 g/cm 3 ) Scintillating fibers ~ 0.5 – 1.0 mm

52 PHENIX calorimeter energy resolution Sep,3 2013A.Kiselev 1mm fibers + ~2mm thick tungsten plates -> poor energy resolution at small incident angles!

53 PHENIX calorimeter energy resolution Sep,3 2013A.Kiselev 1mm fibers + ~1mm thick tungsten plates -> with 1mm plates energy resolution becomes acceptable

54 Summary Sep,3 2013A.Kiselev

55 Sep,3 2013A.Kiselev While smearing generator is still the main physics simulation tool for the group, EicRoot development is in a good progress and code is already suitable for several types of studies: detector acceptance tracking resolutions e/m calorimeter design optimization First physics simulations in EicRoot framework should become possible really soon Other immediate code development goals include implementation of IR (material and fields) implementation of PID algorithms (RICH, TPC dE/dx, …)

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