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Laser Spectroscopic Determination of the Nuclear
Charge Radius of 6He
Prepared by Robert V.F. Janssens and Zheng-Tian
Lu for the DNP webpage
For physicists the nucleus 6He, with
2 protons and 4 neutrons, has been intriguing for quite some time.
Measurements in the eighties and nineties have indicated that,
when used as a beam, the probability for it to induce a nuclear
reaction on any target is much larger than that for 4He.
This observation was interpreted as a strong indication that 6He
is a three-body "halo" nucleus, i.e., it can be best
viewed as a well bound 4He core and 2 neutrons orbiting
this core at large distances. Moreover, while these three constituents
of 6He form a bound system, the nuclear potential is
not strong enough to bind any two of them separately. For this
reason, 6He is often referred to as "Borromean"
(The name derives from the heraldic emblem of the medieval princes
of Borromeo, three rings interlocked in such a way that the removal
of any of the rings will cause the remaining two to fall apart).

Because of its intriguing properties, 6He
has the potential to teach us about the fundamental forces among
the constituent nucleons. Indeed, the halo character can be revealed
by an accurate determination of the nuclear charge radius, since
the motion of the core with regard to the center of mass reflects
both the radial extent of the neutrons and the correlations between
these particles. The result can in turn be compared with the most
modern theories
as recent advances in computational methods have made it possible
to calculate the structure of few-nucleon systems from the basic
interactions between the constituents.
The charge radius of 6He has been
determined for the first time by measuring the atomic isotope
shift between 6He and 4He using laser spectroscopy.
For this work, 6He atoms were produced at the ATLAS
accelerator facility at Argonne National Laboratory, and quickly
captured and cooled by an on-line laser trap. By applying laser
spectroscopy on the trapped 6He atoms as well as on
their 4He isotopic partner atoms, the charge radius
of the 6He nucleus was determined to be 2.054 ±
0.014 fermi, approximately two millionth of a nanometer. The measurement
is of such accuracy that it distinguishes between the available
theoretical predictions. The data offer new insight into the dependence
of three-body interactions on neutron number, which in turn is
essential to the understanding of the structure of all neutron-rich
systems, including neutron stars.

Method: Production and Laser Trapping of 6He
Atoms
In this work, 6He nuclei were produced
via the 12C(7Li, 6He)13N
reaction with a 100 pnA, 60 MeV beam of 7Li from the
ATLAS accelerator at Argonne National Laboratory. Neutral 6He
atoms diffused out of the hot graphite target and were transferred
in vacuum to the nearby atomic beam assembly at a rate of approximately
one million per second. Trapping helium atoms in the 23S1 metastable
level was accomplished by exciting the 23S1
– 23P2 transition using laser light
with a wavelength of 1083 nm. 6He atoms were mixed
with a krypton carrier gas and sent through a discharge to be
excited to the 23S1 level. The metastable
6He atoms were transversely cooled, decelerated with
the Zeeman slowing technique, and then captured in a magneto-optical
trap at a rate of approximately one atom per minute.
This work is supported by the U.S. Department of Energy, Office
of Science, Office of Nuclear Physics, under contract W-31-109-ENG-38.
Reference
Laser Spectroscopic Determination of the 6He Nuclear
Charge Radius. L.-B. Wang et al., Phys. Rev. Lett. (2004) Preprint
(nucl-ex/0408008)
Related Link
www-mep.phy.anl.gov/atta/