1. 4/17/2005FOCUS / Doris Kim1 Doris Y. Kim University of Illinois Urbana-Champaign Content ( hep-ex/0410037, PLB 607 (2005) 233 ) Part I: Theories of charm semileptonic decays. Part II: Reconstructing D 0  K   + and    +  Part III: q 2 dependence, f + (q 2 ) a. Deconvolution approach: Non-parametric analysis. b. Parametric fit. Part VII: Summary Measurements of q 2 Dependence of D 0  K   + and    +  Form Factors. APS Meeting April 17, 2005 Tampa, FL

2. 4/17/2005FOCUS / Doris Kim2 I: Charm semileptonic decay as tests of LQCD The decay rates are computed from first principles (Feynman diagrams) using CKM matrix elements. Charm SL decays provide a high quality lattice calibration, which is crucial in reducing systematic errors in the Unitarity Triangle. The techniques validated by charm decays can be applied to beauty decays. The hadronic complications are contained in the form factors, which can be calculated via non-perturbative Lattice QCD, HQET or quark models.  etc.

3. 4/17/2005FOCUS / Doris Kim3 The lattice community is actively fixing the situation and calculating f+ as a function of q 2. hep-ph/0408306 PRL 94 (2005) 011601 Theories of D  Pseudoscalar l  decays But a major disconnection exists between experiment and theory. In the past, theories worked best where experiments worked worst. cleanest theory highest rate is the easiest point for LQCD calculation. P at rest in D frame Simple kinematics  Easy to extract form factors.

4. 4/17/2005FOCUS / Doris Kim4 Until quite recently, one required a specific parameterized form to bridge the gap between a theory and an experiment, since neither an experiment nor a theory had clean f + (q 2 ) information. Now we have enough data, hence, What do we measure? (old) ISGW1 Method I: f + (q 2 ) shape obtained non-parametrically by deconvolution. Method II: Or fit f + (q 2 ) using specific forms. (old) pole modified pole f + (q 2 ) parameterization ISGW2 Updated version. Spin 1 D* S

5. 4/17/2005FOCUS / Doris Kim5 A good muon candidate. Cerenkov ID for K/  candidates. Good CL ’ s for D production/decay vertices, and L/  > 5 between two vertices. D* tag required, and wrong sign soft    subtraction  II. Reconstructing D 0  K   + and    +  Selection ~ cut rs-ws MC ws 12,840 K   + Neutrino Reconstruction K  rest frame The D and D* mass constraints  the neutrino lies on a cone around the soft pion. Pick the  that points the D closest to the primary vertex. /GeV/c 2

6. 4/17/2005FOCUS / Doris Kim6 III.a q 2 dependence: Deconvolution approach. We actually use a 10  10 matrix A deconvolution matrix is constructed from the number of events generated in the i- th q 2 bin that end up reconstructed in the j-th q 2 bin. This matrix is then used to correct data for resolution and efficiency.

7. 4/17/2005FOCUS / Doris Kim7 Correcting for charm backgrounds in D 0  K   + The background only affects the highest q 2 bins. After subtracting known charm backgrounds, f + (q 2 ) is an excellent match to a pole form with m pole = 1.91  0.04  0.05 GeV/c 2 or  = 0.32 (CL 87%, 82%).

8. 4/17/2005FOCUS / Doris Kim8 III.b Parameterized f + (q 2 ) for D 0  K   + /    + 6574 K   +  events 288    +  events 2-dim fit: cos  l, q 2 Signal ~ MC with reweighted intensity. Backgrounds are floated within known uncertainties.  D0D0 W  rest frame ll

9. 4/17/2005FOCUS / Doris Kim9 Comparing to Lattice Gauge Result K   +

10. 4/17/2005FOCUS / Doris Kim10 Other q 2 information in D 0  K  l  /   l   l  pole mass is  l Kl It disfavors ISGW2 form by ~4.2  form factor f+(q²) single-pole model Based on 820 events q² / GeV² Kl  l Cleo 2004  l  pole mass is Preliminary study

11. 4/17/2005FOCUS / Doris Kim11 Summary of D 0  K  l    l   Results Clearly the data does not favor the simple Ds* pole Kl New world average for K  l  New world average for   l 

12. 4/17/2005FOCUS / Doris Kim12 Question slides