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Bs Ds K

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Bs Ds p- (2.76 0.25) 10-3 from BD- p Bs Ds(*)- K (2.0 0.6) 10-4 from BD- K ... Recently a new vertex fitter was introduced: Lagrange Global Fit ... – PowerPoint PPT presentation

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Title: Bs Ds K


1
Bs ? Ds() K ()
  • Plans for reconstructing Bs ? Ds() K ()
  • Modes
  • Bs ? Ds K
  • Bs ? Ds K
  • Bs ? Ds K
  • and
  • Bs ? Ds p

2
Branching fractions
Estimated branching fractions Bs ? Ds p-
(2.760.25) 10-3 from B?D- p Bs ? Ds()-
K (2.00.6) 10-4 from B?D- K Bs ? Ds() K-
(2.71.0) 10-5 from B?Ds p- (ratio
VubVcs/VcbVus0.37) Bs ? Ds- K (3.71.2)
10-4 from Bs?Ds-K using fK/fK (1) Bs ? Ds
K- (1.70.7) 10-5 from Bs?Ds()K- using
ratio(1) (1) Heavy flavours II, Non-leptonic
weak decays of B mesons, Neubert Stech
3
Subsequent decays
Ds ? K K- p (4.4) Ds ? Ds ?
(94.2) mDs1968.6 MeV Ds p0
(5.8) mDs2112.4 MeV (diff143.8
MeV) K ? K0 p (67) Of which half
decays to Ks0 K p0 (33)
4
Bs ? Ds K
  • Recent work done only on Bs ? Ds K and Bs ? Ds p
  • Used in TP, Reoptimization TDR, several theses.
  • Recently, I tuned the preselection cuts.
  • No analysis yet on Bs ? Ds K and Bs ? Ds K
  • First plan is to try Bs ? (Ds?Ds ?) K, since
  • asymmetry is expected same as Bs ? Ds K
  • reconstruction efficiency same
  • maybe soft photon is not needed to be
    reconstructed

5
Bs ? Ds K
What happens when photon is not
reconstructed? One can calculate the invariant
mass of the Ds K 5008 lt MDsK lt 5313 MeV 300
MeV mass window probably to big to reject enough
background (also Bs ? Ds- p) But it can be
used as pre-selection (no need to try to find
?). Trick Knowing the Ds- mass, and the
primary vertex, there are enough constraints to
fit the whole decay chain (so this includes the
momentum of the B, missing photon etc.)
6
Bs ? Ds K
  • What happens if the p0 or Ks0 are not
    reconstructed?
  • K ? Ks0 p 2256 lt MDsp lt 4546 MeV
  • K ? K p0 3437 lt MDsK lt 5234 MeV
  • Conclusion cannot select decay when p0 or Ks0
    are not found.
  • Maybe decay chain trick works.?

7
Global vertex fit
  • Recently a new vertex fitter was introduced
  • Lagrange Global Fit
  • Based on Lagrange multiplier method
  • Vertex is also implemented as a constraint
  • Mass constraints can be added
  • Pointing constraints can be added
  • Very generic, the whole decay chain can be
    fitted at once.

e.g. two tracks vertex constraint
8
Bs mass plots
Normal fit DsK invariant mass
Invariant mass plots with missing photon.
Calculated correction from constraints.
Global fit photon has huge error
9
Ds resolution
Normal mass constrained fit
Global mass constrained fit
x resolution
z resolution
? the normal mass-constraint vertex fit was wrong
for 3-particle vertices (there were only 2 vertex
constraints instead of 3).
10
LoKi
LoKi Toolkit to make selection of and
looping over Particles, and monitoring easier.
  • Workflow
  • Make the Particles (place particle ID cuts)
  • Run LoKi algorithm to do the combinatorics(presel
    ection or final cuts)
  • Run the efficiency algorithm (acceptance, reco
    and selection eff)
  • Re-do trigger
  • Tag the selected decay
  • Run another LoKi algorithm to fill tuples and
    histograms(optionally tighten cuts)
  • Save to (Mini)DSTWhen running over MiniDST only
    step 6 is needed.

11
Outlook
  • New in Bs ? Ds K - tagging (find
    efficiency) - multiple PVs per event - new
    pre-selection
  • About half of the decays have 1 or more short
    tracks. ?Try to select also these decays in Bs ?
    Ds() K ()
  • Determine pre-selection and final cuts for Bs ?
    Ds K
  • Determine efficiency on signal and background
  • Determine tagging and trigger efficiency
  • Determine resolutions (decay time)
  • Try to reconstruct Bs ? Ds K
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