APS April Meeting 2021
Volume 66, Number 5
Saturday–Tuesday, April 17–20, 2021;
Virtual; Time Zone: Central Daylight Time, USA
Session K03: Laser Based Tests of Fundamental Physics
1:30 PM–3:18 PM,
Sunday, April 18, 2021
Sponsoring
Units:
DAMOP GPMFC
Chair: Alexander Sushkov, Boston University
Abstract: K03.00001 : Precision Microwave Spectroscopy of the Positronium n $=$ 2 Fine Structure
1:30 PM–2:06 PM
Live
Preview Abstract
Abstract
Author:
David Cassidy
(University College London)
Since positronium (Ps) atoms are composed only of leptons they are, for all
practical purposes, pure QED systems and can therefore be used to perform
rigorous tests of bound-state QED theory. Moreover, since the theoretical
description is limited only by the order of the calculations performed,
rather than unknown physical constants or incalculable terms, any observed
(and confirmed) disagreement with theory could indicate the existence of
``new physics'' such as particles or fields not currently included in the
Standard Model.
In this talk I will describe some new measurements of the Ps n $=$ 2 fine
structure intervals. The experiments were performed using a buffer gas
positron trap which allows a dilute Ps gas with a number density on the
order of 10$^{\mathrm{6}}$ cm$^{\mathrm{-3}}$. A pulsed dye laser was used
to optically excite atoms to the 2 $^{\mathrm{3}}$S$_{\mathrm{1}}$ level,
and microwave radiation was used to drive transitions to the 2
$^{\mathrm{3}}$P$_{\mathrm{J\thinspace }}$levels (J $=$ 0,1,2), which decay
radiatively to the ground state before annihilation. The different
annihilation decay rates of the ground and excited (S) states allows the
fine structure transitions to be monitored via the time spectrum of the Ps
annihilation radiation.
We found that the measured J $=$ 1 and J $=$ 2 lineshapes exhibited
significant asymmetries, whereas a symmetric lineshape was observed for the
J $=$ 0 transition. The observed asymmetries are not consistent with the
most obvious quantum interference or line-pulling phenomena arising from
nearby (off-resonant) transitions, and in the absence of a complete
lineshape model we are therefore unable to determine the fine structure
intervals for these transitions. Since the J $=$ 0 lineshape did not exhibit
any significant asymmetry it was possible to extract a value for the centre
frequency: however, the obtained interval was found to disagree with theory
by 2.77 MHz, which amounts to 4.5 standard deviations. No mechanism for a
line shift of this magnitude has so far been identified.