Charm (meson) Semileptonic Decays
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Charm (meson) Semileptonic Decays Jim Wiss University of Illinois (Urbana) Representing FOCUS PowerPoint PPT Presentation


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Charm (meson) Semileptonic Decays Jim Wiss University of Illinois (Urbana) Representing FOCUS. Outline Interference in D +  K pmn FOCUS New D +  K *mn/ K2 p BR CLEO and FOCUS Prognosis for new SL results. New results on D +  K pmn. WS-subtracted.

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Charm (meson) Semileptonic Decays Jim Wiss University of Illinois (Urbana) Representing FOCUS

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Charm meson semileptonic decays jim wiss university of illinois urbana representing focus

Charm (meson) Semileptonic Decays

Jim Wiss

University of Illinois (Urbana)

Representing FOCUS

  • Outline

  • Interference in D+ Kpmn

  • FOCUS

  • New D+ K*mn/K2p BR

  • CLEO and FOCUS

  • Prognosis for new SL results


New results on d k pmn

New results on D+ Kpmn

WS-subtracted

Our Kp spectrum like everyone else’s looks like 100% K*(890)

This has been “known” for about 20 years.

Data

Fit

charm bkg

RS-WS

events

Right Sign

Wrong Sign

21,370events

backgrounds are pretty small

MKp (GeV/c2)

But a funny thing happened when we tried to measure the form factor ratios by fitting the angular distributions ...


Five observables are studied

Five observables are studied

A 4-body decay requires 5 kinematic variables: Three angles and two masses.

MKp

MW2 q2 t

left-handed m+

right-handed m+

Two amplitude sums over W polarization

(“mass terms”)

Wigner D-matrices

H0(q2), H+(q2), H-(q2) are helicity-basis form factors computable by LGT


An unexpected asymmetry in the k decay

An unexpected asymmetry in the K* decay

Yield 31,254

dataMC

We noticed an forward-backward asymmetry in cosqV below the K* pole, but almost none above the pole.

HUGEasymmetry!

Sounds like QM interference


Simplest approach try an interfering spin 0 amplitude

Simplest approach — Try an interfering spin-0 amplitude

(plus mass terms)

A exp(id) will produce3 interference terms

We simply add a new constant amplitude : A exp(id) in the place where the K* couples to an m=0 W+ with amplitude H0.


Since a b interference will dominate

Since A << B, interference will dominate..

There will only be three terms as mm=> 0

If we average over acoplanarity we only get the first term

  • This is the term that created our forward-backward asymmetry!

  • If our model is right:

  • The asymmetry will have a particular mass dependence:

  • The asymmetry should be proportional to sin2ql

  • The asymmetry should have a q2 dependence given by q2 H02(q2)


Studies of the acoplanarity averaged interference

Studies of the acoplanarity-averaged interference

Extract this interference term by weighting data by cosqV

Since all other c-averaged terms in the decay intensitty are constant or cos2qv.

We begin with the mass dependence:

Efficiency correction is small

Our weighted mass distribution..

..looks just like the calculation..

A=0

A constant 450 phase works great...

...but a broad resonance is fine as well.

0.36 exp(ip/4)


Dependence of asymmetry on cos q l

Dependence of asymmetry on cosql

  • We plot the asymmetry versus cos ql and expect a parabola in cos2 ql since sin2 ql = (1 - cos2 ql)

A=0

0.36 exp(ip/4)

Looks  - (1 - cos2 ql). Some modulation due to efficiency and resolution


Q 2 dependence of asymmetry

q2 dependence of asymmetry

Below the pole

A=0

0.36 exp(ip/4)


Acoplanarity dependent interference terms

Acoplanarity dependent interference terms

The interference adds two new terms to the acoplanarity dependence.

Without s-wave interference, the acoplanarity terms are even in c:Only cos cand cos 2cdependencies are present

The interference producessin cterms which breakc to -csymmetry


Our first brush with sin c was frightening

Our first brush with sinc was frightening!

Same sign convention used for D+ and D-

Yikes! CP violation?

Opposite sign convention used for D+ versus D-

Interference with the new amplitude breaks c to -c symmetry.

When CP is handled properly, the D+ and D- acoplanarity distributions become consistent.


The correct acoplanarity convention

The correct acoplanarity convention

counter clockwise about

The sine of the acoplanarity requires 5 vectors to specify

Under CP : D+ => D- , all 5 vectors will reverse as will sin c under our convention. Interference produces a “false” CP violation between the acoplanarity distribution between D+ versus D- unless we explicitly take c to -c


But surely an effect this large must have been observed before

But surely an effect this large must have been observed before?

Although the interference significantly distorts the decay intensity....

...the interference is nearly invisible in the Kp mass plot.


New results on d k mn k2 p branching ratio

New results on D+ K*mn/K2p branching ratio

— RS— WS

Quoted resultfrom this sample


The cleo result might resolve an old problem

The CLEO result might resolve an old problem

The recent CLEO number raises this width considerably .. thus partially resolving this long standing problem.

G(K*l n)/G(Kpp)


The preliminary focus result

The preliminaryFOCUS result

Still under study!

We multiply muon results by 1.05 to compare to electron results

Our preliminary number is 1.59 standard deviations below CLEO and 2.1 standard deviationsabove E691

0.620.02

G(K*l n)/G(Kpp)

muons

electrons

Preliminary


Summary

Summary

(1) S-wave interference inD+ Kpmnof form

The new amplitude is small:7% of BW peak amplitude in the H0 part. 6% of all Kpmn over the full Kp range

  • (2) New results onD+ K*mn/K2p

    • CLEO value 0.74  0.04  0.05 (is higher than previous data)

    • FOCUS preliminary value is 0.60  0.01  0.02 (1.57s lower than CLEO)

  • (3) Many interesting results are on the way:

    • New measurements ofDs+fmn/fp

    • New rv and r2form factor measurements for K*mn and fmn

    • f(q2) measurement forD0  Kmn

    • Cabibbo suppressed ratios: D+ rmn/K*mn & D0 pmn/Kmn


Fmn br work in progress

fmn BR — work in progress

— data— charm background MC

Once we demand a decay out of the target segments, the backgrounds are matched by our Monte Carlo.

This is a “c,cbar” MC with events containing a fmn decay excluded.

Work is being done on the branching ratio measurement, and I hope to work on the form factor measurement.

Perhaps we will see interference with the f0(980)?


Question slides

Question slides


The preliminary focus result1

The preliminary FOCUS result

FOCUSpreliminary(uses the S-wave MC)

G(K*l n)/G(Kpp)

If we were to multiply the FOCUS muon result by 1.05 to compare with CLEO electrons, CLEO would still lie 1.59 standard deviations above FOCUS

Preliminary


Observation of interference in d semileptonic decay into k m n

Observation of interference in D+ semileptonic decay into K* m n

  • I intended to measure several semileptonic form factors as a thesis

    • D+K*0mn was intended as training exercise forthe more controversial Ds+fmn

  • We could not get good confidence level fits on K*0mn, even after exhaustive checks of MC and possible backgrounds

    • Known backgrounds were small and benign (in form factor variables)

    • The Monte Carlo simulated both resolution and acceptance well.

  • We then made a crucial observation that led to an explicit interference model

    • The model is described by only a single amplitude and phase

    • The model explained the discrepancies between the data and the fit.

    • And suggested numerous new places to search for interference


The decay rate via feynman rules

The decay rate via Feynman rules

  • Assuming the Kp spectrum contains nothing but K*,the decay rate is straight-forward

H+, H0, H- are helicity-basis form factor amplitudes.

Form factors describing the hadronic structure are contained in Dmn


Decay rate as an amplitude

Decay rate as an amplitude

Written as an |amplitude|2, the decay rate is much more simple and intuitive:

left-handed m+

(“mass terms”)

right-handed m+

~2%

Wigner D-matrices

internal sum overW polarization

Form factordetails fromFeynmancalculus

Rich + detailed kinematic structure! Angular distributions are highly correlated.


A problem with k l n form factor fits

A problem with K*ln form factor fits!

K*mn is supposed to have just even power terms of cos qv

But the data seemed to require a linear cos qv term below the K* pole and none above the pole.

Yield 31,254

dataMC

We hit upon an interference explanation for a linear cos qv with a dramatic mass dependence.


Did e791 see it

Did E791 see it?

Digitized data from E791 paper. They see an asymmetry in same direction at about 1.5 s level.

Digitized E791 data

If we bin our data like E791 we see a 6s asymmetry with a consistent slope. But even with our huge data sample the effect looks rather subtle.

E831 binned/cut as E791


Beatrice

BEATRICE??

BEATRICE also uses a narrow Kp mass cut, and here the slope of the residuals is 1.2s, in the direction of our effect. So BEATRICE seems to see a hint of this effect as well.


But a broad resonant amplitude works just fine

..but a broad resonant amplitude works just fine.

We can mimic the cosV dependence for a constant amplitude using a BW put in with a relatively real phase.For example use a wide width (400 MeV) and center it above the K* pole (1.1 GeV).

cos qV term


Mass dependence of this interference term

Mass dependence of this interference term

  • To study the c dependence of interference term we use a Fourier weighting of cos(c+d) and sin(c+d) of the Kp mass distribution. This picks out pure interference terms that vary sinusoidally as c and that do not change sign with cos qv . Given the form of the dominant term, we expect:

  • cos(c+d) weighting will pick out the real part of the K* BW

  • sin(c+d) weighting will pick out the imaginary part of the K* BW


Mass dependence of the acoplanarity interference

Mass dependence of the acoplanarity interference.

0.36 exp(ip/4)

A=0

0.36 exp(ip/4)

A=0

The data is in fair agreement with our model and resemble our naive expected shapes. Fractional error bars are large due to the smallness of thesin c and cos c Fourier components that are even in cos qv


Resolution study

Resolution study

Traditional solution

Blanking sample

  • Blank out the softest pion in DK3p and reconstruct it like a neutrino using DVFREE upstream vertex.

  • Compare with “right” answer from reconstructed pion.


Cut variants

Cut Variants

0

8

tkf — TRKFIT CL > 1%


Split samples

Split Samples


Phase of 45 0 mass versus width of s wave

Phase of 450: mass versus width of s-wave

allowedregion


Implications

Implications

Our data is consistent with an interference of the (approximate ) form:

The new amplitude is small: About 7% of the BW peak amplitude in the H0 piece.

  • How would an interfering amplitude affect form factor measurements?

    • -in process of evaluating this but fit quality improves dramatically

    • -might effect the overall scale of the form factors derived from the branching fraction Kpmn/K2p

  • What could be the strength of an s-wave amplitude according to theory?

    • -a small NR-K* interference (~10%) has been predicted by B. Bajc, S. Fajfer, R.J. Oakes, T.N. Pham (1997) hep-ph/9710422

    • Amundson and Rosner, Phys. Rev. D47, (1993) 1951

  • Will there be similar effects in other charm semileptonic or beauty semileptonic channels?

  • -Good question!


Cuts to eliminate non charm backgrounds

Cuts to eliminate non-charm backgrounds


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