Click here for NTUPLE format description (132-column text file).
New column-wise ntuples were made for the optimized analysis by Greg Landsberg. Reduced row-wise ntuples (RWNs) are being made by Dan Karmgard and Pushpa Bhat. Following triggers were used for data ntuples
Column-wise Ntuples:
All of them are also available on dafm04::tmp$root355:[pushpa.dan.enujj.ntuples]
I. Available files (Number of Events)
1) In PRJ$ROOT215:[NEW_PHENOM_1.GREG.EVJJ]
a) LQ160.NTP (1999)
LQ180.NTP (1999)
LQ200.NTP (1999)
LQ220.NTP (4996)
NEWNT_1A_1.NTP (2831)
NEWNT_1B_1.NTP (3073)
NEWNT_1B_2.NTP ()
NEWNT_1B_3.NTP ()
NEWNT_1B_4.NTP ()
* Ntuples with no events listed were recovered, and will be
written to this directory shortly.
2) In prj$root261:[new_phenom_6.greg.top_jets]
a) TOP_LJ170_A.NTP (4996)
TOP_LJ170_B.NTP (5094)
TOP_LJ170_C.NTP (4950)
TOP_LJ170_D.NTP (4906)
TOP_LJ170_E.NTP (4913)
TOP_LJ170_F.NTP (4924)
TOP_LJ170_G.NTP (5044)
TOP_LJ170_H.NTP (4954)
TOP_LJ170_I.NTP (4998)
TOP_LJ170_J.NTP (4950)
3) In prj$root261:[new_phenom_6.greg.top_leptons]
a) TOP_LL170_A.NTP (13527)
TOP_LL170_B.NTP (13791)
TOP_LL170_C.NTP (13232)
TOP_LL170_D.NTP (13356)
TOP_LL170_E.NTP (13329)
TOP_LL170_F.NTP (8966)
TOP_LL170_G.NTP (8894)
TOP_LL170_H.NTP (7609)
TOP_LL170_I.NTP (9150)
TOP_LL170_J.NTP (9280)
4) In prj$root261:[new_phenom_6.greg.wjj]
a) WJJ_1.NTP (1390)
WJJ_2.NTP (21191)
II. Row wise Ntuples (Made from Gregs' columnwise sets) for RG
Search and Neural Networks are on the Alpha cluster in
TMP$ROOT355:[PUSHPA.DAN.ENUJJ.NTUPLES]
A) Available Files (Number of Events)
1) LQEV_160.RWN (865)
LQEV_180.RWN (898)
LQEV_200.RWN (937)
LQEV_220.RWN (2396)
DATA_1A.RWN (198)
DATA_1B.RWN (305)
TOP_LJ_MT170.RWN (22251)
TOP_LL_MT170.RWN (52428)
WJJ.RWN (10050)
B) Cuts applied to Gregs' ntuples to make the RWN.
1) Bad Run Veto (Data and QCD only)
2) NMu = 0 OR (NMu > 0 AND Mu_OK = 0) for each Muon
3) Missing ET > 20
4) Revertexing information available
5) One EM object with
a) ET > 20
b) |Eta| < 2.5 but
c) not 1.1 < |Eta| < 1.5
6) Electron ID Cuts (data only)
a) 5 Variable likelihood < 1.0
b) chi squared < 100
c) isolation < 0.15
7) 2 through 5 Jets in the event with
a) Jet EMF < 0.95
b) |Eta| < 2.5
c) ET > 15
d) ej Cone > 0.2
8) Missing ET seperated from the two leading jets by at least
0.25 in phi. 0.25 < |dPhi| < PI-0.25
Monte Carlo Generation
III. Guoliangs' Ntuples are located on the Alpha Cluster in
PRJ$ROOT341:[NEW_PHENOM_6.SCRATCH.WANGGL.MC_CWN]
A. Files Available (Number of Events) (Cross Section) (BR)
1) LQNUE_40.CWN (2000) (819)
LQNUE_60.CWN (1999) (111)
LQNUE_80.CWN (1999) (24.7)
LQNUE_100.CWN (2000) (7.38)
LQNUE_120.CWN (2000) (2.65)
LQNUE_130.CWN (2000) (1.67)
LQNUE_140.CWN (1999) (1.08)
LQNUE_150.CWN (1999) (0.711)
LQNUE_160.CWN (1999) (0.79300)*
LQNUE_180.CWN (1999) (0.37319)*
LQNUE_200.CWN (1999) (0.18420)*
LQNUE_220.CWN (4996) (0.09320)*
LQNUE_240.CWN (4997) (0.04853)*
LQNUE_250.CWN (1998) (0.03529)*
* => NLO Cross Section.
2) TOP_LJETS170T_HW057_01.CWN +
TOP_LJETS170T_HW057_02.CWN (82244) (5.77) (0.454)
TOP_TTLL170XS_HW057_01.CWN +
TOP_TTLL170XS_HW057_02.CWN (101339) (5.77) (0.0685)
W2L80AJHE_VB300_G315TZ3_01.CWN +
W2L80AJHE_VB300_G315TZ3_01.CWN +
W2L80AJHE_VB300_G315TZ3_01.CWN +
W2L80AJHE_VB300_G315TZ3_01.CWN (345296) (810.7) (1)
B. Guoliangs' Cuts for the standard analysis.
1) ZVertex1 < 50
2) Missing ET > 40
3) Muon exclusion
4) 1 Electron with
a) ET > 25
b) |Eta| < 1.2
5) 2 Jets with
a) ET > 25
b) |Eta| < 1.0
c) Third jet allowed with ET > 25 and |Eta| < 2.5
6) Electron seperated from all jets by dR > 0.25
7) Electron ID cuts on data only
a) 4 Variable likelihood < 0.25
b) Electron isolation < 0.10
8) Missing ET seperated from all jet axes by 0.25
9) HT = Sum(Jet ET) + Electron ET
10) Transverse mass of electron neutrino pair > 100
11) dM/M (Hobbs variable) < 0.2