Lattice meets experiment: (g-2) Brendan Casey, Fermilab Conclusions - - PowerPoint PPT Presentation

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Lattice meets experiment: (g-2) Brendan Casey, Fermilab Conclusions - - PowerPoint PPT Presentation

Lattice meets experiment: (g-2) Brendan Casey, Fermilab Conclusions The determination of (g-2) m to 0.54 ppm has yet to be confirmed Therefore we cant believe it The 0.44 ppm error in the predicted value is dominated by


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SLIDE 1

Lattice meets experiment: (g-2)

Brendan Casey, Fermilab

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SLIDE 2

Conclusions

5/6/1 1 2/15

  • B. Casey, USQCD all hands

s

  • The determination of (g-2)m to 0.54 ppm has yet to

be confirmed

– Therefore we can‟t believe it

  • The 0.44 ppm error in the predicted value is

dominated by non-perturbative QCD

– Therefore we can‟t believe it

  • We need to re-determine (g-2)m of the muon to

higher precision with a new experiment

– Goal is 0.14 ppm

  • We need a rigorous, non-perturbative calculation

that predicts the value of (g-2)m that can be verified using independent data.

– Goal is set by experimental precision

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SLIDE 3

Overview

  • Was on the organizing committee of Lattice meets

experiment 2010 workshop at Fermilab

  • Was asked to give a „perspectives from an

experimentalist‟s point of view‟ at this all hands meeting

  • In both cases, I agreed if I would be allowed to

shamelessly plug the new g-2 experiment

  • I would like to give my impressions and get people

motivated to work on g-2

5/6/1 1 3/15

  • B. Casey, USQCD all hands

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SLIDE 4

Impressions: Bs mixing

5/6/1 1 4/15

  • B. Casey, USQCD all hands

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D D + CDF D + CDF D + CDF + improved z

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SLIDE 5

Impressions: Bs mixing

5/6/1 1 5/15

  • B. Casey, USQCD all hands

s

D D + CDF D + CDF D + CDF + improved z

Lesson learned: Lattice is just as important as experiment

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SLIDE 6

Impressions: Kp puzzle

5/6/1 1 6/15

  • B. Casey, USQCD all hands

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5 s difference between CPV in K+p- and K+p0 Basically useless because no solid prediction Similar situation for g-2 “In principle….”

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SLIDE 7

Impressions: Kp puzzle

5/6/1 1 7/15

  • B. Casey, USQCD all hands

s

5 s difference between CPV in K+p- and K+p0 Basically useless because no solid prediction Similar situation for g-2 “In principle….”

Lesson learned: estimates, models, and symmetries are great until you disagree with what you expect

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SLIDE 8

Impressions: fb

5/6/1 1 8/15

  • B. Casey, USQCD all hands

s

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SLIDE 9

Impressions: fb

5/6/1 1 9/15

  • B. Casey, USQCD all hands

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B factories

Btn

CKM

fD, fB Dln DK

Spectroscopy spectroscopy mixing mixing

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SLIDE 10

Impressions: fb

5/6/1 1 10 10/15

  • B. Casey, USQCD all hands

s

B factories

Btn

CKM

fD, fB Dln DK

Spectroscopy spectroscopy mixing mixing

Lesson learned: everything takes a long time so figure out what you need before you start and get everyone on board Working together = enormous success

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SLIDE 11

Muon G-2

  • “We just don‟t understand QCD at that level.”

– This is almost a community wide consensus

  • LO effects like vacuum polarization can be taken from
  • data. But higher order effects like hLbL so far cant.

– hLbL is predicted to be the dominant error in the next

  • round. Apparently a „killer‟ for prioritization committees.
  • No lattice people on P5!
  • Spin is fundamental. QCD is fundamental. “We just

don‟t understand” is completely unacceptable.

– You have to add “yet”

  • Electron g-2 is considered the crowning achievement
  • f QED

– Muon g-2 could be the crowning achievement for QCD

5/6/1 1 1 1 1 1/15

  • B. Casey, USQCD all hands

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SLIDE 12

G-2 status

  • BNL measurement to 0.54 ppm
  • Fermilab expects 0.14 ppm
  • Dominant sys:

– Backgrounds from p‟s

  • 10x longer decay channel

– Pileup in the calorimeters

  • Finer segmentation
  • Stats:

– Booster rep rate >> AGS rep rate

  • Fermilab = 20x total BNL stats

in about 1 year

  • The experiment is mostly built, the

collaboration exists, the director loves it, and the DOE is on board.

– This is happening

5/6/1 1 12 12/15

  • B. Casey, USQCD all hands

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SLIDE 13

Program: g-2

5/6/1 1 13 13/15

  • B. Casey, USQCD all hands

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  • Fermilab:

– Same as BNL but better

  • JPARC:

– Completely different technique, competitive precision

  • KEK, INFN:

– Possible to do g-2 of t via t+t- spin correlations

@ 75 ab-1: s(at)~ 5 x10-6

Bernabau, Gonzalez-Sprinberg, Videl JHEP 0901:062 (2009)

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SLIDE 14

Program: e+e-

5/6/1 1 14 14/15

  • B. Casey, USQCD all hands

s

QCD

m m g p e g e hadrons

KLOE BaBar

e g e hadrons

g

New experiments this decade

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SLIDE 15

Program: tau

5/6/1 1 15 15/15

  • B. Casey, USQCD all hands

s

e g e p + p - t W p + p 0 n tau and e+e- data are converging with time. ~3s difference now ~2s t data set will increase by more than a factor of 100 this decade compared to published results

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SLIDE 16

Program: gg

5/6/1 1 16 16/15

  • B. Casey, USQCD all hands

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KLOE has added detectors down-stream of the collision point to tag

  • utgoing e+ and e- from two

photon collisions

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SLIDE 17

Possible combined program

5/6/1 1 17 17/15

  • B. Casey, USQCD all hands

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muon g-2 measurements independent measurements Lattice

tau spectral function R scan radiative return electron g-2 two photon BNL FNAL JPARC

QCD

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SLIDE 18

Conclusions

5/6/1 1 18 18/15

  • B. Casey, USQCD all hands

s

  • The determination of (g-2)m to 0.54 ppm has yet to

be confirmed

– Unacceptable

  • The 0.44 ppm error in the predicted value is

dominated by non-perturbative QCD

– Unacceptable

  • We need to re-determine (g-2)m of the muon to

higher precision with a new experiment

– Short term goal is 0.14 ppm

  • We need a rigorous, non-perturbative calculation

that predicts the value of (g-2)m that can be verified using independent data.

– In principle we can do this.