Closed manuelfs closed 2 weeks ago
For the $\phi$-enriched sample, the cuts/weights the angular analysis use are essentially the DD cut/weight times this: $1015 \lt m_{KK} \lt 1023$ MeV + oppositely charged tracks (and require long tracks).
Thanks for finding their cuts.
He calls them pions, but since they pass ProbNNk_Greater
cuts and the main way to reconstruct $\phi$ mesons is via their $\phi \rightarrow KK$ decay, I think they are kaons.
Yeah, you're right, I just wasn't thinking. Edited my comment
Working on finishing the yml file up with all these things included, and then I'll start the step-2 production, but first to check: are the HLT flags/weights you're referring to just k_hlt1_trackmva_tos(_emu)
, pi_hlt1_trackmva_tos(_emu)
, d0_hlt1_twotrackmva_tos(_emu)
? Because these are already included in our step-2 tuples.
Ah, great. I checked the yml file, and it doesn't have the emu
versions, but I now realize that they may be added via auxiliary files.
I committed a first version of the weights for the proton sample with the Brunel_MC15TuneV1_ProbNNp > 0.4
cut. This i the PID variable that we use for protons in the misID unfold. I also added a few words about PID weights to the README
.
I'm thinking that the weights will be different for the D**
if we want to use them to mock up the Lambdas
.
By the way, I noticed that wskim_dd_new
is not consistent with is_dd_new
due to a missing GhostProb cut.
I checked the DDX
truthmatching. It now separates 4 kinds of DDX
adding up the codes here. The code looks good.
On a pure DDspi
file like 11894400
, 100% of events satisfy truthmatch == 120000
, as expected.
On a D0mu
sample DDX
file like 11894600
, I get
given the breakdown of decays in the .dec
file shown below, the truthmatching seems indeed fine if we allow for the DDspi
efficiency to be about twice as high as for the other modes, and the DD
efficiency to be lower.
dd_3body_k = 10000; --> 52.12% of total
0.10951 MyOtherD*- MyD*0 K+ PHSP;
0.07331 MyD*- MyOtherD*0 K+ PHSP;
0.05011 MyD*+ MyOtherD*- K0 PHSP;
0.03990 MyD*+ MyD- K0 PHSP;
0.03062 MyD*- MyOtherD*0 K*+ PHSP;
0.03062 MyD*+ MyOtherD*- anti-K*0 PHSP;
0.02320 MyD- MyD0 K*+ PHSP;
0.02320 MyD- MyD*0 K*+ PHSP;
0.02227 MyD*0 MyOtheranti-D*0 K0 PHSP;
0.01856 MyD*- MyOtherD0 K+ PHSP;
0.01670 MyD*- MyD+ anti-K0 PHSP;
0.01670 MyD*- MyOtherD0 K*+ PHSP;
0.01578 MyD*+ MyD- anti-K*0 PHSP;
0.01021 MyD0 MyOtheranti-D*0 K0 PHSP;
0.00993 MyD- MyD0 K+ PHSP;
0.00928 MyD*0 MyOtheranti-D*0 K*0 PHSP;
0.00464 MyD*0 MyOtheranti-D0 K0 PHSP;
0.00464 MyD0 MyOtheranti-D0 K*0 PHSP;
0.00464 MyD0 MyOtheranti-D*0 K*0 PHSP;
0.00464 MyD*0 MyOtheranti-D0 K*0 PHSP;
0.00278 MyD0 MyOtheranti-D0 K0 PHSP;
dd_2body_Ds = 2000; --> 35.85% of total
0.10951 MyD*- MyD_s*+ SVV_HELAMP 0.4904 0.0 0.7204 0.0 0.4904 0.0;
0.05754 MyD*+ MyD_s1- SVV_HELAMP 0.4904 0.0 0.7204 0.0 0.4904 0.0;
0.04919 MyD*- MyD_s+ SVS;
0.03898 MyD_2*- MyD_s+ STS;
0.03712 MyD_2*- MyD_s*+ PHSP;
0.02227 MyD_1- MyD_s*+ SVV_HELAMP 0.48 0.0 0.734 0.0 0.48 0.0;
0.01114 MyD'_1- MyD_s*+ SVV_HELAMP 0.48 0.0 0.734 0.0 0.48 0.0;
0.01114 MyD_1- MyD_s+ SVS;
0.00928 MyD*+ MyD_s0*- SVS;
0.00557 MyD'_1- MyD_s+ SVS;
0.00371 MyOtherD'_s1- MyD+ SVS;
0.00306 MyD*+ MyD'_s1- SVV_HELAMP 0.4904 0.0 0.7204 0.0 0.4904 0.0;
dd_34body_pi = 20000; --> 10.95% of total
0.03434 MyD_s*+ Myanti-D0 pi- PHSP;
0.03434 MyD_s+ Myanti-D0 pi- PHSP;
0.02042 MyD_s*+ Myanti-D0 pi- pi0 PHSP;
0.02042 MyD_s+ Myanti-D0 pi- pi0 PHSP;
dd_2body = 1000; --> 1.07% of total
0.00508 MyD*+ MyOtherD*- SVV_HELAMP 0.47 0.0 0.96 0.0 0.56 0.0;
0.00377 MyD*- MyD+ SVS;
0.00188 MyD*+ MyD- SVS;
I added the variable phi_m
with the invariant mass of the two least isolated opposite-charge long tracks. Alex added useful branches to select a phi
-enriched sample in data (is_phi
) and in MC (wphi
).
Running over 10 data files we get a phi
peak similar to Run 1's (Fig. 119 in the ANA note), albeit with a bit more background.
Since the cuts are the same as in the dd
skim, the kaon may not be actually used to form the invariant mass. If we wanted less background we could require that 1 or 2 of the tracks in the invariant mass satisfy the kaon PID, but that would require calculating new weights and performing a standalone fit, so it is easier to keep the dd
selection.
Events in the 1015 < phi_m < 1023
mass region are 1-1.5% of the total events in the dd
skim, depending on the PID cuts.
I checked the branches in D0mu
sample DDX
MC 11894600
as well.
A new production of step 2 ntuples is needed with the following features
px
/py
/pz
, remove truep
/pt
DDspi
eventsDDspi
to be 10% ofD*
DDX
eventsphi
-enriched sample with two oppositely charged kaons, inv. mass compatible withphi
(and weights for MC)