1 in the meantime... 1. varied p t cut (1.5 gev, 1 gev, 500 mev) 2. allowed for events with 2 good...

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1 In the meantime ... 1. Varied p T cut (1.5 GeV, 1 GeV, 500 MeV) 2. Allowed for events with 2 good tracks only (+), originally 4 good tracks where required, in order to fully reconstruct the B S D S () decay 3. Enlarged angle cuts , between K + and K : 10 13 deg (see next slide) 4. changed from CDF fitter to VKal fitter 5. Used reprocessed data (r1093) 6. Applied the analysis to MC Min.Bias sample

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Page 1: 1 In the meantime... 1. Varied p T cut (1.5 GeV, 1 GeV, 500 MeV) 2. Allowed for events with 2 good tracks only (+  ), originally 4 good tracks where required,

1

In the meantime ...

1. Varied pT cut (1.5 GeV, 1 GeV, 500 MeV)

2. Allowed for events with 2 good tracks only (+),originally 4 good tracks where required,in order to fully reconstruct the BSDS() decay

3. Enlarged angle cuts , between K+ and K:10 13 deg (see next slide)

4. changed from CDF fitter to VKal fitter

5. Used reprocessed data (r1093)

6. Applied the analysis to MC Min.Bias sample

Page 2: 1 In the meantime... 1. Varied p T cut (1.5 GeV, 1 GeV, 500 MeV) 2. Allowed for events with 2 good tracks only (+  ), originally 4 good tracks where required,

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What we presently do/plan to do

Do background subtraction by using same sign combinations of tracks.

Find more appropriate function for describing the background shape (polynomial has stability problems with low statistics).

The fitting function for signal should better be a Breit-Wigner accounting for phase space convoluted with a Gaussian to represent the detector resolution.

Go down only to pT > 0.8 GeV, and build a phi peak again (still no dE/dx). Make a mass plot of () candidates, that build a 3-prong vertex, look at the DS

meson mass region (putting both + and candidates into one plot).

last time we said:

Page 3: 1 In the meantime... 1. Varied p T cut (1.5 GeV, 1 GeV, 500 MeV) 2. Allowed for events with 2 good tracks only (+  ), originally 4 good tracks where required,

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Width of the (1020) in MC truth

width [GeV] mass [GeV]

PDG 1990 4.41 1998 4.43 2006-9 4.26 1019.46

Pythia_6.42 4.43 1019.4(current version) PMAS(KC,2) PMAS(KC,1)

Fitting the Monte Carlo truth signal with a Breit-Wigner (relativistic and non-relativistic) gives m = 1019.38 0.004 GeVand = 4.45 0.01 GeV, which is larger than the current PDG value investigations

Conclusion: (1020) in ATLAS Monte Carlo productionsnot generated with the current PDG value for the width!

Page 4: 1 In the meantime... 1. Varied p T cut (1.5 GeV, 1 GeV, 500 MeV) 2. Allowed for events with 2 good tracks only (+  ), originally 4 good tracks where required,

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Fit

Page 5: 1 In the meantime... 1. Varied p T cut (1.5 GeV, 1 GeV, 500 MeV) 2. Allowed for events with 2 good tracks only (+  ), originally 4 good tracks where required,

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Fitting the (1020) signal

Using a convolution of a Breit-Wigner with a Gaussian (and a threshold function for the bg) inside the RooFit framework

has already implemented this convolution: “Voigtian“– fix width of Breit-Wigner ( = 4.26 GeV)

RooVoigtian signal("signal","Voigtian PDF",x,mean,width,sigma); width.setVal(4.26); width.setConstant(kTRUE);RooGenericPdf bg("bg","background","(x-987.35)^p*exp(-b*(x-987.35))",RooArgSet(x,p,d));

RooAddPdf model("model","sum of signal and bg",RooArgList(signal,bg),RooArgList(Nsig,Nbkg));model.fitTo(data); // Extended Maximum Likelihood Fit (unbinned)width.Print();

Page 6: 1 In the meantime... 1. Varied p T cut (1.5 GeV, 1 GeV, 500 MeV) 2. Allowed for events with 2 good tracks only (+  ), originally 4 good tracks where required,

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Comparision with the old method

N = 60.7 15 = 2.93 0.74

N = 58 16 = 2.88 0.76

N = 76 19Gauss = 1.8 1.0

One gets 30% more events(due to tails of Breit-Wigner).

with first plot shown(pT > 1.5 GeV)

Gauss

Gauss Voigt