499c
Nuclear Physics A446 (1985) 499c-5OOc North-Holhd, Amsterdam
Connnent on
:
A-EXCITATIONIN NUCLEI
Michele ROY-STEPHAN IPN-Orsay,
BPl,
and Laboratoire
F-91406 Orsay National Saturne,
Going
A physics,
on
with
developments
I
CEN Saclay,
would like to say a few words
of a program concerning
at Saturne.
This program
has started
by an experiment
LNS collaboration. to spin-isospin
F-91191 Gif-sur-Yvette
Cedex on
further
A in nuclei via charge exchange reactions
is devoted to spin isospin excitation on (3He,t)
in a
Copenhagen,
in general, and
Lund, Lyon, Orsay,
In (3He,t) spectra, the complete response of the nucleus
probe
has shown
up
: nuclear particle-holes
time. Moreover
excited
at the same
13He,t)
: the A peak in nuclei is shifted 70 MeV down in energy with respect
to the free A excitation, collective
cancellation charge
between
exchange
is
The
(u,q)
various unique
region
the maximum
would
still
separated.
be The
measurements. deuteron
and
effects
by the virtual
if
step
response
Saturne.
our
The
It will
experimental
it
(AS = 1
1).
AL =
Another
be
will
A excitation
provide
ion physics. in an heavy
assume that A excitation
037%9474/85/$03.30
high
- and
where energy
precisely,
using
Very
2He)
sensitivity
thus
the
which
ion reaction
could
involve
tensor state
be
spin
polarized
interaction
at 0" or at small angle.
is
assignment
much
as an (z, c)
more
advantageous
n and p contributions. should
for
give
a
of Gamov-Teller spin
dipole
(n,p)
definitive strength.
transitions
of freedom has long remained unexplored,
recently,
dominate
is very close
The
responses
will
in S = 0 final
to separate
measured,
spin
process
matter.
nearly as much information (2,
domain opened to A degrees
heavy
reaction
answer to the question of the quenching
Furthermore,
one,
respect,
transverse
program
protons
will bring
will
and
in a spectrometer
be possible
strength
transverse
this
II:exchange
research
two
together
T22 measurements
Gamow-Teller
In
in nuclear
longitudinal
of
reaction and in the present situation
i.e.
occurs.
: n and p can both contribute
spanned
be detected
experimentally.
of the
sensitive to medium effects.
improved
of
in
in nuclei. Strong medium effects are expected
spin-isospin
next
has appeared
(fig. 1). It raises the question
We will study the (a, 2He)
beam
(2He), will T20
of
feature
response, but not in the z x G
virtual n are especially
to
pt3He,t)A++
nature of A excitation
in the a.{ longitudinal
a very intriguing
and A have been
we have observed, (fig. 2).
n production
QEkvie.r Science Publishen B.V. (North-Holland Physics Publishing Division)
It seems
for the first
time,
very reasonable
to
in heavy ion. It is also a very
M. Roy-Stephan / A-Excitation in nuclei
E=950
MeV/A
27AL(20Ne,
E=950
b)
0'
20Na)
MeV/A
0)
0”
T+,i,o,(GeV) FIGURE 1
FIGURE 2
important energy. the
mechanism
for thermal
We will thus undertake
very
peripheral
nature
equilibration a detailed
of this
in heavy
ion reactions
investigation
reaction,
we will
at high
of this process. Using have access
to density
effects. Another
problem
direct TI emission, would
deserves
give an answer.
intensities. injector,
This
: how does a A deexcite in a nucleus,
It would
further
holes ? Coincidence
need big solid angle detectors
direction
implies
operation
Mimas, which will also offer the possibility
reactions,
as
Relying
the
exchange
attention
coupling with 2 particle-2
on
for
we think
correlations.
example
very direct that
heavy and
ion
simple
H.I.D.C.I.
double
charge
character
should
of
measurements
and higher beam the
new
Saturne
of studying more exotic exchange
of heavy
be a sensitive
(H.I.D.C.I.).
ion single
charge
probe of short range