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Outline Detectors and Methods Spectrometer layout Segmented target, OOT cut effectiveness CITADL • Kaonicity pion ID effect on K-pi reflection Target Silicon Vertexing and skim strategy Omega signal EM Calorimeters & Muon Upgrades IE & OE pi0 reconstruction D*-D mass Semileptonic Physics Form Factor Measurement D0-D0bar mixing FOCUS Physics K K Ks Dalitz DCSD : D+ -> KKK Charm baryon signals CascadeC -> p k pi LambdaC -> sigma pi pi Double-D Production K K pi Dalitz D lifetimes CP Violation and Mixing D0 CP eigenstate lifetime diffs. CLEO plots FOCUS Advantages K-pi signal Skim Strategy (candidate- driven) CP asymmetry (Daniele) CP asymetry (O’Reily)

Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

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Page 1: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

Outline• Detectors and Methods

– Spectrometer layout– Segmented target, OOT cut

effectiveness– CITADL

• Kaonicity• pion ID effect on K-pi

reflection– Target Silicon– Vertexing and skim strategy– Omega signal

• EM Calorimeters & Muon Upgrades– IE & OE

• pi0 reconstruction– D*-D mass– Semileptonic Physics

• Form Factor Measurement• D0-D0bar mixing

• FOCUS Physics– K K Ks Dalitz– DCSD : D+ -> KKK– Charm baryon signals

• CascadeC -> p k pi• LambdaC -> sigma pi pi

– Double-D Production– K K pi Dalitz– D lifetimes

• CP Violation and Mixing– D0 CP eigenstate lifetime diffs.

• CLEO plots• FOCUS Advantages• K-pi signal• Skim Strategy (candidate-

driven)

– CP asymmetry (Daniele)– CP asymetry (O’Reily)

Page 2: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

Segmented TargetD

ecays/2

00

m Be

OBeO

tarsil

tarsil

black - primary vertex red - secondary vertex

• 62% of D decays occur in air• Out-of-Material cut virtually eliminates non-charm backgrounds

From background subtracted charm!

Page 3: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

D+ Yield = 11528 S/N = 2.8

p( )M KK

DKK

p( )M KK

D+ Yield = 7157 S/N = 10

Out of Material

Page 4: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

“Kaonicity” Golden Kaons & pions

Likelihood based Cerenkov algorithm

Page 5: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

D+ +- without Cerenkov ID

K reflection

signal

Page 6: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

D+ +- with loose pion IDp- >1.0KW W

Yield = 3317

Page 7: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

D+ +- with tight pion ID

Yield = 2092

p- > 4.0KW W

Page 8: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

0 reconstruction with the IE and OE

Y ield = 1 0 7 1 4S/N = 1 5

(with D* tag)

D0 K-+0

Page 9: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

2 0( )M

2( )M K

*K

*0 0K

0K

D0 K-+0 has a rich substructure with lots of interference

Page 10: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

Target Silicon Detector

20

25

30

35

40

45

50

5800 7800 9800 11800 13800run number

Proper time resolution vs run number

TS used

No TSTS inst

alle

d

ts ( )fs

Target Silicon detector improves proper time resolution by about 20%

Page 11: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

D*-D Mass Difference Measurements• These measurements hilight our improved 0

reconstruction• Statistical errors should be about 3 times better than

present world average

*0 0( ) ( )M D M D

*0 0 0 0,D D D K

= 142.02 0.03 MeV

PDG = 142.12 0.07 MeV

M

* 0,D D D K

*( ) ( )M D M D

= 140.72 0.03 MeV

PDG = 140.64 0.10 MeV

M

Page 12: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

c pK

Charm Baryon Signals

Cabibbo suppressed decay mode of the

(first observed by SELEX)

c

Page 13: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

2GeV/c 2GeV/c

c c c

Page 14: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

Expected resonance contributions to D0 KKKS

Class 1 BSW requires resonance coupling to u-dbar quarks and a dikaon. The only resonances are:

•a0 (980) (sub-threshold)

•a2 (1320)Class 2 BSW requires resonance coupling to u-ubar quarks and a dikaon:

f0 (980) (subthreshold)

•f2 (1270)

Page 15: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

2( )SM K K

2( )M K K

lobes

0(980) ?a

0(980) ?f

2( ) (GeV/c )sM K KK

Dalitz Analyses SD K K K

Page 16: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

FOCUS Semileptonic Physics

• Measure Form Factors for

– Check against recent LGT calculations

• Cabibbo suppressed decays:• Semileptonic mixing:• Rare or forbidden decays:

Expect roughly 50 times more semimuonic events than E687 with our rebuilt muon system!

*0

*0s

s

D K

D

D

De eK

0D l D lr n p n+ ® ®* 0 0 ( )D D D Kp mp p n+ + ++ + -® ® ®

0D mm+ -®

Page 17: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

*0 ( )D K K

— Right Sign — Wrong Sign

RS-WS yield 56445

( )M K

Page 18: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

D0 CP eigenstate Lifetime Differences

CLEOassuming CP

CLEO allowi

ng CP

violation

M

Page 19: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

FOCUS can make competitive measurement

0 signal from FOCUSD K K

Y=16532 STN=2.3

Expect y =1.3%

(y (CLEO) = 1.73%)

M(KK)

Page 20: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

• Extremely good proper time resolution : 8% (D0)

– No resolution systematics or error inflation

• A segmented target with ~62% of decays verticizing in air

– Grossly minimizes absorption corrections in matter

• Excellent (and flexible) Cerenkov identification

– Vary misidentification reflections to gauge systematics.

• Skims use a vertexing algorithm with nearly flat t’ acceptance

– Minimizes any reliance on MC and reduces systematic error

• We expect to measure y to within 1.3%

FOCUS ADVANTAGES

Page 21: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

Skim Strategy with minimal time bias

K

KSeed track

Primary vtx track

Recoil charm track

Nearly uniform time acceptance --right up to the skim cut!

Nucleate about seed track to form a primary vertex.

Look for two tracks with a good intersection

A minimum bias skim for D0 KK

Page 22: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

CP Violation Search in D+ and D0 Decays

0

0Where( ) ( ) ( )

( ) ( ) ( )

( )CP

D D N D K KA D

D D N D K

D KK D KK D

Asymmetry mechanism in PythiaNeed to correct for production asymmetry which occurs at ~3% level

Page 23: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

*D *DExpecting 1-2% sensitivity

Page 24: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target
Page 25: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

Doubly Cabibbo Suppressed Decays

D Peak DS PeakD = 8.5 MeV/c2

DS = 8.5 MeV/c2

D KKK

Page 26: Outline Detectors and Methods –Spectrometer layout –Segmented target, OOT cut effectiveness –CITADL Kaonicity pion ID effect on K-pi reflection –Target

Double D Photoproduction Dynamics

Charm and anticharm acoplanarity distribution probes NLO QCD

The correlation between a charm particle and an anticharm particle in the same event

radians)

: kinematic tag

: Double D reconstruction ~