Difference between revisions of "Main Page"

Latest revision as of 16:58, 8 February 2024

Welcome to the Jefferson Lab Positron Working Group

Mission: The mission of the positron working group is to explore and develop the capabilities for positron beam physics at Jefferson Lab.

News! To join the mailing list please send an e-mail to pwg-request@jlab.org with the word "subscribe" in the subject field. Contact Joe Grames (grames@jlab.org) or Eric Voutier (voutier@ipno.in2p3.fr) for any concern related to the JLab PWG.

Announcements

Archived Documents

Meetings

PAC Proposals

Working Groups

Consult the User's Guide, Configuration settings list and MediaWiki FAQ for information on using the wiki software.

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-<strong><big>Welcome to the Wiki of the Jefferson Lab Positron Working Group (Pwg@jlab.org)</big></strong>
-Consult the [//meta.wikimedia.org/wiki/Help:Contents User's Guide], [//www.mediawiki.org/wiki/Special:MyLanguage/Manual:Configuration_settings Configuration settings list] and [//www.mediawiki.org/wiki/Special:MyLanguage/Manual:FAQ MediaWiki FAQ] for information on using the wiki software.
+<font size="10">
+<div style="text-align: center;">
+'''Welcome to the Jefferson Lab Positron Working Group '''
+</div>
-== <strong>Interference Physics</strong> ==
+<font size="5">
+<div style="text-align: center;">
+'''Mission''': The mission of the positron working group is to explore and develop the capabilities for positron beam physics at Jefferson Lab.
+</div>
-''Coordinators: John Arrington (johna@anl.org), Charles Hyde (hyde@jlab.org)''
+<font size="4">
+<div style="text-align: center;">
+'''News!''' To join the mailing list please send an e-mail to pwg-request@jlab.org with the word "subscribe" in the subject field.  Contact Joe Grames (grames@jlab.org) or Eric Voutier (voutier@ipno.in2p3.fr) for any concern related to the JLab PWG.
+</div>
-The effort of this sub-group is to consider the benefits of the application of polarized positrons in the electromagnetic physics sector. In the energy range currently available at JLab, ther is no specific difference with respect to the scientific information obtained with an electron or a positron probe. However, when more than one QED-based mechanism contributes to a reaction process, the comparison between lepton beams of opposite charge allows one to uniquely distinguish the quantum interference between these mechanisms. This feature is expressed in the experimental measurement of the electromagnetic form factors of the nucleon where two-photon exchange mechanisms may reconcile cross section and polarization data, and also in the experimental measurement of the generalized parton distributions of the nucleon where the interference between the Bethe-Heitler and virtual Compton amplitudes is a key observable.
+<!--[[Image:epluseminus.png|thumb|200px|alt=Group Photo.|Text goes here.]]-->
-== <strong>Charged Current Physics</strong> ==
+'''[[Announcements]]'''
-''Coordinator: Wally Melnitchouk (wmelnitc@jlab.org)"
+'''[[Archived Documents]]'''
-== <strong>Test of the Standard Model</strong> ==
+'''[[Meetings]]'''
-''Coordinators: Marco Battaglieri (battaglieri@ge.infn.it), Xiaochao Zheng (xiaochao@jlab.org)"
+'''[[PAC Proposals]]'''
-== <strong>Positron Applications</strong> ==
+'''[[Working Groups]]'''
-''Coordinator: Tony Forest (tforest@jlab.org)"
+<font size="3">
-Positron annihilation spectroscopy (PAS) is a well-known technique for investigating the structural properties of materials. because of the purity of the 2<math>\gamma<\math> signal produced from the annihilation of positrons with atomic electrons, this technique is a very sensitive probe of material defects and constitutes an accurate method for the measurement of the momentum distribution of electrons. Nevertheless, the globally poor availability of intense positron beams at low energies (1-1000 keV) percludes efficient use of PAS. An MeV electron accelerator production of positrons, like that used in the PEPPo experiment, can easily provide two orders of magnitude greater beam intensities than the most powerful nuclear reactor based facility. Adding controlled and flexible polarization capabilities with the PEPPo technique at accelerator facilities, may constitute a technological breakthrough for PAS and help address the lack of low energy positron research facilities world-wide.
+Consult the [//meta.wikimedia.org/wiki/Help:Contents User's Guide], [//www.mediawiki.org/wiki/Special:MyLanguage/Manual:Configuration_settings Configuration settings list] and [//www.mediawiki.org/wiki/Special:MyLanguage/Manual:FAQ MediaWiki FAQ] for information on using the wiki software.
-== <strong>Positron Production and Beam Physics</strong> ==
-''Coordinators: Joe Grames (grames@jlab.org), Vasiliy Morozov (morozov@jlab.org)"
-The efficient transfer of polarization from electrons to positrons (>80%) has been demonstrated by the PEPPo experiment and offers a new pathway to use low energy polarized electron beams (10-100 MeV) to promptly produce polarized positrons suitable for acceleration. A challenging aspect of the positron injector is the optimization required to achieve the desired beam characteristics, such as beam intensity, transverse emittance (size), bunch length and energy spread (longitudinal emittance) necessary and be well-mated to the accelerator design (e.g. 12 GeV CEBAF, LERF, JLEIC). A core activity of this sub-group is to evaluate the user requirements, accelerator integration and assess the merits and risks of different schemes appropriate for JLab, in order to summarize and recommend the R&D needed for a successful positron physics program.

Difference between revisions of "Main Page"

Latest revision as of 16:58, 8 February 2024

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