exclusive d s semileptonic decays using kinematic fitting
Post on 19-Dec-2015
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Exclusive Ds Semileptonic decays using kinematic
fitting
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Analysis Techniquese+ e- (1--)
Ds+* (Ds
+) + ...Ds-(Ds
-*)
e+ and K*0(K+-) e+
SIGNAL SIDE
TAGGED SIDE:
+ CC Event
Ks
K+K-)-
+--
K*K*(KsK-+-)-
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Analysis Techniques• Define the beam constrained mass:
• Cut “loose” on Mbc then look at the invariant mass. We do NOT require one candidate per event based on “best” Mbc since Mbc and the invariant mass are correlated.
• Evaluate missing mass-squared (MM2) on the signal side:
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Exclusive Ds semileptonic decays 4
Selection criteria
Track Quality Cuts:
• Hit fraction > 0.5• Good fit• |d0|<0.5cm and |Z0|<5.0cm• |cosθ| < 0.93 • |p| >0.04 GeV
Particle ID
• Both dE/dX & RICH PID if |p| > 0.7GeV,
• dE/dX PID if |p| < 0.7
PID for the 1st and/or 2nd kaon. | Mass-PDG|<0.02
GeV
PID for Pion and kaon. | Mass-PDG|<0.100
GeV
e
electron ID.|p| > 0.2GeV.FRICH ≥ 0.8
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Kinematical constraints
•
•
•
• • Mass of the tag is constrained to the DS mass
• Total of 7 constraints
• 4 Missing variables in the fit (Energy and Momentum of the ).
• 2 is then determined for both -tag or -he hypotheses for any legitimate photon candidates.
2 2 2 2
*
(2.1121) (1.9683) (2.1121) (1.9683)
4* 4*Ds beam Ds beambeam beam
E E or E EE E
*S S
beam D D2E =E +E
*SS
DDM -M =143.6 MeV
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MM2 resolution improvements Fitted
Not fitted
Ds+ e+ nu K+- mass [0.7761,0.9761] GeV
Ds+ e+ nuK+K- mass [1.010,1.030] GeV
Signal
MC
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Invariant mass of Ds tag
KsK-
Inv Mass (GeV)
-
Data
K*K* from KsK--
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MM2 for Ds+ e+
Ds+ e+ nuK+K- mass [1.010,1.030] GeV
MM2 [GeV2] m [GeV]
Inv mass
Data
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MM2 for Ds+K*0 e+
Ds+ e+ nu K+- mass [0.7761,0.9761] GeV
Inv mass
MM2 [GeV2] m [GeV]
Data
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Next …
• Will remove the PID on the K in K*(Kπ).
• Get effect on effeciencies.
• Get the branching fractions.
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Generic MC(1)
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Generic MC(2)
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Generic MC(3)