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Michelangelo D’Agostino UC Berkeley Madison Meeting April 2008

Detecting Atmospheric Neutrino-Induced Cascades with IC-22.  e. Michelangelo D’Agostino UC Berkeley Madison Meeting April 2008. Outline. Level 2 Cuts further cascade reconstructions two new cuts based on split reco. Level 3 Cuts Containment Cuts how close are we to detection?.

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Michelangelo D’Agostino UC Berkeley Madison Meeting April 2008

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  1. Detecting Atmospheric Neutrino-Induced Cascades with IC-22 e Michelangelo D’Agostino UC Berkeley Madison Meeting April 2008

  2. Outline • Level 2 Cuts • further cascade reconstructions • two new cuts based on split reco. • Level 3 Cuts • Containment Cuts • how close are we to detection? Really Close!!

  3. Event Rates At Filter Level • ≈1500 eC.C. after the Pole filter for 200 days • ≈3000 e C.C.+ N.C. after the Pole filter for 200 days • we have closer to 240 days of livetime

  4. Level 2 Cuts Proposed Level 2 Cuts: 83% signal efficiency (atm.) 81% background rejection 

  5. Level 2 Cuts: Neural Net Total Paraboloid Error

  6. Level 2 Cuts: Neural Net Level 2 Cuts Used In This Talk: 80% signal efficiency (atm.) 84% background rejection

  7. Level3: MPE Cascade Reconstruction • Level 2 processing uses SPE UPandel with re-coincified hits • Using the full hit series and seeding MPE UPandel with the SPE result is better Note: Plot is after Level 2 cuts

  8. Level 3: MPE Cascade Reconstruction Note: Plot is after Level 2 cuts

  9. MPE Cascade Reconstruction X Resolution [m] Y Resolution [m] Note: Plots are weighted for an atmospheric flux and post Level 2 cuts with no containment MPE RMS’s (atm.): x: 20.4 m y: 18.7 m z: 9.7 m Z Resolution [m]

  10. Hit in early half Track Cascade Hit in late half Level 3: Split Cascade Reco Basic Idea: 1. Split hit series in two around the average time (cf. coincident muon reconstruction) 2. Reconstruct each half as a cascade Two (un-correlated) parameters which should be good: Distance between the two vertices, and the time difference between the two vertices.

  11. z time Level 3: Split Cascade Reco. z is more powerful than xy because of DOM spacing more effective for coin. muons Note: Plots are after Level 2 cuts

  12. Level 3: 32-Fold Track Reconstruction Note: Plot is after Level 2 cuts

  13. Containment Cuts Note: Plots are after Level 2 cuts Signal Data is much more concentrated around the outer edges of the detector than signal is. 8 hr Data

  14. Spatial Significance Plot cut? 78% signal eff. (atm.) 94% background rej. Containment Cuts Spatial Significance Plot

  15. Tentative Cuts Summary • Online Filter: 1/(1+2+3) and vlf • 34% signal eff., 97% background rej. • Level 2: single and Lsingle-LcscdSPE • 83% signal eff., 81% background rej. • Level 3: z , LcscdMPE, and 32 • 81% signal eff., 76% background rej. • Level 4: XY-Containment, (Z Containment?) and time • 78%*74% signal eff., 94%*59% background rej. Still to explore: Energy reconstruction

  16. scaled up from 8 hours of data, so immune to potential MC problems

  17. Conclusions • common Level 2 cuts are set • Level 3 reconstructions (+Rime) are generally agreed upon • processing of the full dataset will begin very soon • none of the cuts I’ve presented are optimized or finalized (indeed, most are only a few weeks old), and more are in the pipeline • we’re getting very close to where we need to be to make a first detection of -induced cascades!!

  18. scaled up from 8 hours of data, so immune to potential MC problems

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