S&C Offline Software

2017-08-31 16:00
2017-08-31 17:00
America/New York
Thursday, 31 August 2017
1-189, SRN, at 20:00 (GMT), duration : 01:00
SRN ID: 1096183

EVO Phone Bridge Telephone Numbers:
---------------
- USA (BNL, Upton, NY)
+1 631 344 6100

- USA (Caltech, Pasadena, CA)
+1 626 395 2112
TimeTalkPresenter
16:00HFT Embedding / Misalignment ( 00:20 ) 0 files
16:20Forward Tracking Progress ( 00:20 ) 0 files
16:40Tracking Optimization ( 00:20 ) 0 files
17:00AOB ( 00:20 ) 0 files

HF PWG Meeting Minutes by Zhenyu - 2017/8/31

1) J/psi v2 in Run12 UU 193 GeV - Alena Harlenderova 

J/psi v2 in UU

FMS sim, trigger phi depdence and gain non-linearity

 This gives an update on some recent work with PSU's local FMS sim.

Parameterized Fit Fuctions for Non-Linearity w/ Radiation Damage

 Fit Data comes from ~10k Pi0 with 3.05<eta<3.15, looking at decay photons.

Two Files Correspond to the two fit functions:

Sector-0006 MWPC test results with Fe55 and X-ray tube

 

Flow decorrelation updates

 

NPE MB Run12 p+p 200 GeV

 

HFT Matching ratio charge dependence

During the checking of D0 and D0bar spectra. we find an interesting performance about the single track  HFT matching ratio do have some charge dependence.

LFS-UPC PWG

2017-08-21 10:30
2017-08-21 12:30
America/New York
Monday, 21 August 2017
, at 14:30 (GMT), duration : 02:00

18th Lomonosov conference. Slides v 6

18th Lomonosov conference. Slides v 5

18th Lomonosov conference. Slides v 4

18th Lomonosov conference. Slides v 3

18th Lomonosov conference. Slides v 2

Simulation Update (Aug 28, 2017)

Speaker : M.H Zhao


Talk time : 13:30, Duration : 00:20

 All results are still single particles today.
 I will show Pythia results next week.

FMS analysis 08/28/2017

2017-08-28 13:30
America/New York
Monday, 28 August 2017
2-78, at 17:30 (GMT), duration : 00:00
 
TimeTalkPresenter
13:30Simulation Update (Aug 28, 2017) ( 00:20 ) 1 fileM.H Zhao

root2agml

First heat map of SS06

We are using a 200 microCi Sr90 source, mounted on an x-y table, to measure the response of the detector as a function of position.  Our 1.2-cm-thick detector (with wrapping) is too thick for any

Conference slides