Irradiation of Polarized Target Materials

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Presentation transcript:

Irradiation of Polarized Target Materials How to Use UITF Irradiation of Polarized Target Materials Chris Keith Target Group December 12, 2018

Irradiation of Polarized Target Materials Solid ammonia (NH3 and ND3) is the most frequently utilized polarized target material at JLab Used in all three halls during 6 GeV era, and intended for use in multiple, approved experiments in A, B, & C at 12 GeV. For successful dynamic polarization, the sample must receive a dose of ionizing radiation (creates NH2 radicals) The optimum dose is about 109 Rad, or 3∙1016 e-/cm2 This is 1.3 hr/cm2 at 1 mA A typical 25 g sample size for irradiation might be 5 cm dia. x 2 cm long 24 hrs @ 1 mA (or 2 ½ hrs @ 10 mA) . Heretofore, all ammonia samples were irradiated and provided by Don Crabb at UVa, but he’s retired now…

Irradiation of Polarized Target Materials . Ammonia freezes at 196 K, and the NH2 radicals recombine at ~130 K, so the irradiation has to be performed at cryogenic temperatures, usually under liquid argon (90 K). In addition to ammonia, other polarized target materials can be prepared by electron-irradiation: LiH and LiD Butanol and propanediol Polystyrene and PMMA Nuclear targets (19F, 23Na…)? Different materials may benefit from irradiation at different temperatures (e.g. LiH @ 180K), so a variable temperature cryostat is desirable.

Irradiation of Polarized Target Materials Variable Temperature Irradiation Dewar Vertical & Rotary Motion Helium gas OUT Helium gas IN Either the beam, or the sample is rastered The beam energy is low, so all unnecessary material should be minimized (windows, etc) LN2 bath Liquid/gas heat exchanger Ammonia sample Thermometers UITF BEAM To Faraday Cup Control Heater

Irradiation of Polarized Target Materials - BACK-UP SLIDES -

Irradiation of Polarized Target Materials Dynamic Nuclear Polarization in a Nutshell Unpaired electrons are implanted in the target sample and polarized at low temperature and high field. eg At 1K and 5 T: Pe ~ 100%, Pp < 1% 5 Tesla Microwaves near the electron resonance frequency induce a simultaneous electron-proton “flip-flop” (or “flip-flip”) The electron quickly relaxes back to its original, polarized ground state The proton relaxes slower, stays in its new spin state ① ② ③ ④ ① ② ③ ④