1 ACD studies: 1. Light Yield Determination for top ACD Tiles 2. Looking for holes (screws) in the ACD data Instrument Analysis Workshop VI Luis C. Reyes.

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Presentation transcript:

1 ACD studies: 1. Light Yield Determination for top ACD Tiles 2. Looking for holes (screws) in the ACD data Instrument Analysis Workshop VI Luis C. Reyes February 28th, 2006 U. of Maryland / GSFC

2 Light Yield Determination for top ACD tiles Procedure Outline: Obtain very clean muon sample -> MIP cuts Select relevant events for LY determination per every channel Calculate efficiency as a function of threshold and fit assuming a poisson distribution for the number of photoelectrons. Data used: B2 and B30 runs -> ~37.4 M triggers digi v3r4p6, recon v3r4p6, svac v3r4p7 Considered to use B2 runs with Muon Kalman hypothesis, but that wouldn't provide enough statistics

3 MIP Selection Cuts ➢ Tkr trigger is present, Tkr opens the trigger window “(GemConditionsWord&2)&&GemCondArrivalTimeTkr==0” ➢ Only one track “TkrNumTracks==1” ➢ Only one MIP found in CAL “CalMipNum==1” ➢ Energy deposition in CAL consistent with MIP “abs(CalMIPRatio-1.)<0.1” ➢ Self-veto gammas by using Tkr hits “Tkr1SSDVeto==0” ➢ Small  2 for the track “log10(Tkr1Chisq)<0” ➢ ~5.3 M ( ~15%) events left after cuts

4 Channel-Specific Cuts ➢ Select events where the only track intersects only the tile under consideration “AcdNumTkrIntSec==1&&AcdTkrIntSecTileId[0]==TILE” ➢ Stick to events “close” to normal incidence by restricting the max path length across the tile “AcdTkrIntSecPathLengthInTile[0]< 10(12) + 2.” ➢ Stay away from the edges: “abs(AcdTkrIntSecLocalX[0])<100&&abs(AcdTkrIntSecLocalY[0])<100” ➢ Cut out events with large error in the point of intersection “log10(AcdTkrIntSecLocalXXCov[0])<1.&&log10(AcdTkrIntSecLocalYYCov[1])<1.” ➢ Only allow events with normal range (range = 0) “AcdRange[TILE][PMT]<1”

5 Efficiency as a function of threshold and number of photoelectrons determination Pulse height distributions for muon sample ✔ Verified MIP peak positions by fitting to a landau distribution convoluted with gaussian. Efficiency = Events over threshold Total Number of Events ✔ From the fit we obtain the mean number of photoelectrons (mean value of the Poisson distribution) AcdPha[32][0]

6 Results A diagram of the ACD with value of PE for every tile goes here

7 Looking for holes (screws) in the ACD Data Existence of holes (screws holding the tile) is one of the distinctive features of the ACD (not in the geometry yet) The very large and “pure” sample of MIPs should be useful to gather some of this information With most of the same cuts as before but allowing events from the edges, let's plot the point of Track+Tile intersection for events with energy deposition in the tile below zero suppression:

8 Number of hole-like events as a function of threshold Tile 33 6 events 7 events 13 events 10 events

9 Holes and leaks in top ACD (threshold at 0.3MIP)

10 Count number of holes in every tile as a function of the threshold (0. MIP, 0.1 MIP, 0.2 MIP,...) Find the average coordinates and RMS for the hole in every corner of every tile Compare to what we expect from the top ACD design: A1B6B4B5C3 K1H5H7H8L3 J1D1D2D4J2 L2 H3H6H1K2 C1B1B7B8A3 Holes (screws) are 3 mm in diameter Top ACD has symmetry with respect to the center Did you know that the holes are not in the same position for every tile? Tiles from the same type have holes in the same position, modulus some rotation Color-coded distribution of tile types in top ACD

11 This tile is flipped along x axis because cables go in +y direction. ~75 mm ~ 35mm ~75 mm Central ACD Tiles

12 Tiles on the sides have screws farther away from the Edge: Left Bottom Corner of top ACD ~95 mm ~35 mm ~95 mm ~60 mm ~75 mm ~35 mm Tile 0Tile 1 Tile 11Tile 10

13 Fraction of hole-like events as a function of Threshold ACD Requirement Likely setting for operations Holes in the tiles is one of the features contributing to ACD inefficiency (gaps, edge degradation, etc...) Given the hole dimensions (3mm diameter x 10 mm length), a muon flux with Cos 2  distribution would yield a fraction of ~2.6 x at 0. MIP ✔ We are in the right ballpark

14 Summary Holes are there :) Their position was determined from the data ➔ This could be useful input for the geometry model Fraction of events going through holes was calculated ➔ Useful comparison to MonteCarlo once holes are modeled Could it be possible to use the hole positions for tile alignment studies? (comparing positions from data with positions from technical drawings) more statistics needed...., systematics?

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