1 / 12

The Precision Muon Group at UW arrived Fall 2010, like many of you

The Precision Muon Group at UW arrived Fall 2010, like many of you. Mulan : G F from m + lifetime MuCap : g P from m - p capture MuSun : m - d capture calibrates basic astrophysics Muon g-2 : anomalous magnetic moment Mu2e: Charged lepton flavor violation test. Faculty

vian
Download Presentation

The Precision Muon Group at UW arrived Fall 2010, like many of you

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. The Precision Muon Group at UWarrived Fall 2010, like many of you • Mulan: GF from m+ lifetime • MuCap: gP from m-p capture • MuSun: m-d capture calibrates basic astrophysics • Muon g-2: anomalous magnetic moment • Mu2e: Charged lepton flavor violation test • Faculty • David Hertzog, Peter Kammel (all projects) • Tianchi Zhou and Alejendro Garcia (g-2) • Postdocs: • Peter Winter, SerdarKizgul FrederikWauters • Graduate Students: • Brendan Kiburg, Sara Knaack, Jason Crnkovic, Michael Murray, Andreas Trautner, + 2 RA-supported SLOTS OPEN David Hertzog: hertzog@uw.edu http://www.npl.washington.edu/muon/

  2. Goal: 0.14 ppm Future Goals Expected Improvement • The New Muon g-2 Experiment at Fermilab • Faculty: David Hertzog, Peter Kammel, TianchiZhou and AlejendroGarcia x10-11 Experiment 3.6 s Theory

  3. p p g m Z m p p B Weak Had LbL Had VP Had VP QED am= (g – 2)/2 is non-zero because of virtual loops, which can be calculated very precisely Known well Theoretical work ongoing The “g-2 test”: Compare experiment to theory. Is SM complete?

  4. difficult to measure at LHC Example: SUSY contribution toaμ:

  5. SUSY and g-2: The power to resolve among models and break LHC degeneracies

  6. Background reduced by x20 Muon storage x10 per proton 20x Events vs BNL in 1 year Ideal muon delivery to storage ring

  7. The Ring Assembly 7

  8. Sikorsky S64F 12.5 T hook weight (Outer coil 8T) 8

  9. n p+ m+ 4 Key elements of the g-2 measurement (1) Polarized muons ~97% polarized for forward decays (2) Precession proportional to (g-2) (3) Pm magic momentum = 3.094 GeV/c E field doesn’t affect muon spin when g = 29.3 (4) Parity violation in the decay gives average spin direction µ 9

  10. The Storage Ring components affect muon storage Fast Kickers Superconducting inflector magnet incoming muons Electrostatic Quadrupoles

  11. digitized samples An “event” is an isolated positron above a threshold. e+

  12. If you find this interesting … • David Hertzog • C533 • hertzog@uw.edu • Peter Kammel • C515 • pkammel@uw.edu • And, you can talk to our current students who are here • Michael Murray (MuSun: transferred to UW) • Andreas Trautner (1st year, exchange; Belle project) • Sara Knaack, Jason Crnkovic, Brendan Kiburg (UIUC)

More Related