Download presentation

Presentation is loading. Please wait.

Published byPaula Erven Modified over 3 years ago

1
G measurement at CB@MAMI Ken Livingston, University of Glasgow, Scotland Slides from: Ken Livingston: Various talks at - http://nuclear.gla.ac.uk/~kl/talks/ David Howdle (ex Glasgow) - /home/davidh/docs/presentations Stuart Fegan (ex Glasgow) - /home/stuartf/Presentations/ Annika Theil (Bonn) - http://nuclear.gla.ac.uk/~baryons2013/Talks/Thiel.pdfhttp://nuclear.gla.ac.uk/~baryons2013/Talks/Thiel.pdf Also talks in this session on Baryons 2013: http://nuclear.gla.ac.uk/Baryons2013/HadSpect1.html

3
Missing baryon resonances

5
Better to look at angular distributions and polarization observables.

6
Polarization observables in pseudoscalar meson production 4 Complex amplitudes: 16 real polarization observables. Complete measurement from 8 carefully chosen observables. πN has high statistics but in KY recoil is self-analysing Pseudoscalar mesons J p = 0 - Here's the nonet of uds ones: + N → m → Y

7
Polarization observables in pseudoscalar meson production 4 Complex amplitudes: 16 real polarization observables. Complete measurement from 8 carefully chosen observables. πN has high statistics but in KY recoil is self-analysing I. S. Barker, A. Donnachie, J. K. Storrow, Nucl. Phys. B95 347 (1975). πNπNKY recoil targ γγ targ recoil ☻☻☻ ☻ linearly polarized photons ☻☻☻ longitudinally polarized target ☻☻☻ transversely polarized target circ polarized photons ☻☻☻ Complete, and over-determined

8
Polarization observables + N → m Linear Polarisation Circular polarisation Nucleon recoil polarimiter x → Y Hyperons are “self analysing” Transverse polarized nucleon targets Longitudinally polarized nucleon targets

9
Polarization observables - a simple example,

10
Systematics of detector acceptance cancel out. “Only” need to know P lin, the degree of linear polarization.

11
'G' is one of the beam-target double polarisation observables, arising from a linearly polarised beam with a longitudinally polarised target In this case, terms not involving linear polarisation of the beam and longitudinal polarisation of the target are zero and the above expression becomes a lot simpler:

12
The effect of G can be seen by examining the asymmetry distribution for positive and negative longitudinal target polarisations The distributions for the positive (top) and negative (bottom) target polarisations show a phase shift due to change in target polarisation By adding distributions for the two target polarisations, the G contribution can be eliminated and a measurement of can be attempted on Butanol If we take similar asymmetries of Kaon azimuthal angle distributions for the Butanol data, the amplitude of a cos(2) fit is not a pure measurement of the observable – it also contains a contribution from the G observable

13
● The A2 Hall is a real photon experimental setup ● It uses a tagged photon beam, which stimulates a reaction within the target cell. A collection of detection systems are then used to measure the reaction products

14
● Electrons scattering of a radiator produce bremsstrahlung photons ● Scattered electrons are bent into an electron focal plane via the Tagger dipole magnet ● The position on the focal plane is used to determine the energy of the bremsstrahlung photon incident on the experimental target

15
● Electrons scattering of a radiator produce bremsstrahlung photons ● Scattered electrons are bent into an electron focal plane via the Tagger dipole magnet ● The position on the focal plane is used to determine the energy of the bremsstrahlung photon incident on the experimental target

16
● Electrons scattering of a radiator produce bremsstrahlung photons ● Scattered electrons are bent into an electron focal plane via the Tagger dipole magnet ● The position on the focal plane is used to determine the energy of the bremsstrahlung photon incident on the experimental target

17
Meson photoproduction with linearly and circularly polarized photons on polarized target FROzen Spin Target (butanol = C 4 H 9 OH)

21
● First step in the reaction identification is to select the π 0 from two photons ● The proton can be selected from the missing mass technique, and its subsequent scattering can be measured

22
Reconstruct the invariant mass of 2 gammas to get pi (and eta) Identify proton in missing mass

25
~200 MeV – ~800 MeV Mainz

27
Shift workers need to pay particular attention to this

Similar presentations

OK

Eurotag Development of the European Tagged photon facilities. Spokesperson: Ken Livingston, Glasgowurl: www.nuclear.gla.ac.uk/~kl/Eurotag Upgrade to 250MeV.

Eurotag Development of the European Tagged photon facilities. Spokesperson: Ken Livingston, Glasgowurl: www.nuclear.gla.ac.uk/~kl/Eurotag Upgrade to 250MeV.

© 2018 SlidePlayer.com Inc.

All rights reserved.

To ensure the functioning of the site, we use **cookies**. We share information about your activities on the site with our partners and Google partners: social networks and companies engaged in advertising and web analytics. For more information, see the Privacy Policy and Google Privacy & Terms.
Your consent to our cookies if you continue to use this website.

Ads by Google

Ppt on depth first search vs breadth Elements of one act play ppt on tv Ppt on writing summary Ppt on life study of mathematician paul Ppt on db2 introduction to accounting Ppt on office automation tools Ppt on carbon cycle in nature Ppt on properties of prime numbers Ppt on sixth sense technology free download Download ppt on management of natural resources class 10