Nucleon-nucleon correlations inside atomic nuclei synergies observations and theoretical models Ranjeet Dalal1 and I.J. Douglas MacGregor2

2025-04-26 0 0 1.95MB 42 页 10玖币
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Nucleon-nucleon correlations inside atomic nuclei:
synergies, observations and theoretical models
Ranjeet Dalal1, and I.J. Douglas MacGregor2
1Guru Jambheshwar University of Science and technology, Hisar, India
2SUPA School of Physics and Astronomy, University of Glasgow, Glasgow G12 8QQ,
United Kingdom
E-mail: ranjeet@gjust.org
August 2022
Abstract. While the main features of atomic nuclei are well described by nuclear
mean-field models, there is a large and growing body of evidence which indicates an
important additional role played by spatially-correlated nucleon-nucleon structures.
The role of nucleonic structures was first suggested by Heidmann in 1950 to explain
pick-up reactions of energetic nucleons. Since then a steady flux of new experimental
evidence has confirmed the presence of similar structures inside atomic nuclei,
dominated by correlations between pairs of nucleons. The role of these internal
nucleon-nucleon correlations has been established using various energetic probes like
photons, pions, leptons and hadrons. These correlated structures are essential for
understanding the interaction of particles with nuclei and their presence provides
an explanation of many specific nuclear phenomena including backscattered protons,
copious deuteron production, sub-threshold particle production, neutrino interactions
with nuclei and the EMC effect. On the theoretical side, these measurements have
stimulated a large number of phenomenological models specifically devised to address
these enigmatic observations. While reviews exist for specific interactions, there is
currently no published commentary which systematically encompasses the wide range
of experimental signatures and theoretical frameworks developed thus far. The present
review draws together the synergies between a wide range of different experimental and
theoretical studies, summarises progress in this area and highlights outstanding issues
for further study.
arXiv:2210.06114v1 [nucl-th] 12 Oct 2022
Nucleon-Nucleon correlations inside atomic nuclei 2
1. Introduction
The internal structure of nuclei has traditionally been investigated using a wide range
of energetic probes, leading to the ejection of one or more nucleons, or to meson pro-
duction. These probes include photons [1], pions [2], electrons [3], protons [4], neutrons
[5] and neutrinos [6]. The interaction of probes with nuclei have provided vital infor-
mation about the state of the nucleus and individual nucleons just before the interaction.
The interaction of energetic photons with nuclei was initially expected to result in
the ejection of individual nucleons [7] from specific shell model orbits. However, the
observed nucleon angular distributions, cross-sections and the ratio of ejected protons
and neutrons measured in early experimental work, led Levinger [8] to conclude that
in many cases more than one nucleon was involved in the interaction. To explain these
unexpected observations, he formulated the simple quasi-deuteron model (QDM) in
which neutrons and protons often occur in deuteron-like structures inside nuclei. The
resulting model, which is at odds with the nuclear shell model, has been quite successful
in explaining the various subtleties of photon interactions with nuclei for Eγabove 40
MeV [9, 10, 11, 12, 13, 14]. In this quasi-deuteron process, the photon-energy absorp-
tion predominantly takes place on a strongly interacting neutron-proton pair while the
remaining nucleons act as spectators, making the (γ, np) reaction an attractive tool to
investigate 2N correlations in nuclei.
The dominance of quasi-deuterons, or spatially correlated neutron-proton struc-
tures inside nuclei, was also confirmed by measurements of charged-pion absorption in
nuclei [2], where absorption on two-nucleon pairs has undergone extensive testing since
the 1950s.
Note that the nature of the correlation, or interaction, between the interacting
nucleons depends on their spatial separation. At long range it is often modelled by
single-pion exchange mechanisms, while at shorter distances it may involve multiple
meson exchange or direct quark or gluon exchanges, if the nucleons are close enough
to overlap. In general, higher energy probes are required to study shorter spatial sep-
arations and the commonly used term Short Range Correlations (SRC) is reserved for
correlations studied with such high energy probes.
Recently, the inclusive and exclusive quasi-elastic reactions (p, p0NN) and (e, e0NN)
have been investigated at very high momentum transfer at BNL [4] and Jefferson Lab
[3], respectively, where the angular correlations between ejected nucleons have been
studied to reveal the state of nucleons just prior to the interaction of energetic probe
particles. For ejected nucleons with momenta above 250 MeV/c, it has been observed
[4] that around 92% of the time protons ejected from 12C targets are accompanied by
correlated neutrons. The most likely explanation is that the emitted high-momentum
Nucleon-Nucleon correlations inside atomic nuclei 3
nucleons originate from short-range spatially correlated nucleon pairs. Such SRCs in-
volving neutrons and protons are similar in construct to the quasi-deuteron concept first
formulated to describe lower energy interactions.
The presence of a significant fraction of nucleons in strongly correlated 2N clusters,
mainly quasi-deuterons or neutron-proton SRCs, leads to many other subtle observations
including enhanced deuteron ejection by energetic probes. Pion absorption reactions [2]
have led to copious deuteron ejection (up to 25% compared to the yield of ejected pro-
tons or neutrons) from nuclei. Similar observations were reported by Baba et al. in
1984 for photons of multi-hundred MeV energies [15]. A significant fraction of energetic
photon and pion absorption events result in either the predominant and simultaneous
ejection of kinematically correlated proton-neutron pairs, or the emission of deuterons.
The presence of nucleon-nucleon correlations inside nuclei was first used to explain
the properties of pickup reactions by energetic neutrons [16]. A notable example is
copious deuteron ejection observed at forward angles by multi-hundred MeV hadrons,
reported in early experiments by Azhgirei et al. [17]. This was understood in terms
of underlying quasi-deuteron degrees of freedom inside nuclei by Sutter et al. [18].
These observations have been confirmed by recent experiments where the coincidence
measurement of elastically scattered protons and deuterons are used to investigate the
spin-isospin character of SRCs at Osaka [19]. The unexpectedly high deuteron pro-
duction, observed in numerous experiments using collisions of multi-GeV relativistic
protons (for example, the early work of Cocconi et al. [20]), may be seen as extension
of Azhgirei and Sutter’s quasi-deuteron propositions.
There have been many other independent manifestations of few-nucleon quasi-
bodies inside nuclei, for example neutrino interactions with nuclei [6, 21], including the
significant fraction of 2-proton emission events [22], the observation of backscattered
protons with unexpectedly high energy for multi-hundred MeV proton beam [23, 24],
the sub-threshold production of particles [25, 26] and the EMC effect [27].
On the theoretical side, there have been intense activities to explain unexpected ob-
servations, most notably the development of the independent pair model or IPAM [28]
and through the high-momentum components of nucleons in an independent particle
framework [3]. The other notable models considering SRCs inside nuclei are the unitary
correlation operator method (UCOM) [29] and recently proposed contact formalism [30].
The present work is an effort to encompass a wide range of experimental investigations
and theoretical works illuminating the correlated structures observed within nuclei. A
holistic review may stimulate further investigations of these phenomena.
Nucleon-Nucleon correlations inside atomic nuclei 4
2. Experimental Indicators
The first evidence for nucleon-nucleon correlated structures inside nuclei appeared
shortly after the availability of energetic beams of photons, neutrons and pions more than
70 years ago. The range of evidence supporting spatially-correlated nucleonic structures
has grown considerably since then. In this section, some of the key experimental
indicators of strong nucleon-nucleon correlations are discussed. Our intention is not
to present an exhaustive review of all the available evidence, but to underscore the
ubiquitousness of correlations observed through a wide and diverse set of experiments.
The most important observations advocating correlated degrees of freedom are:
(i) Interaction of energetic photons with nuclei through the quasi-deuteron mechanism;
(ii) Inclusive and exclusive reactions (e/p, e0/p0NN) using energetic electrons/ protons;
(iii) Pion absorption reactions where absorption of pions takes place mainly through
2N-absorption mechanisms;
(iv) Direct quasi-elastic knockout of deuterons at forward angles using nucleons of a few
hundred MeV energy;
(v) Backscattering of hadrons of several hundred MeV energy from nuclei and sub-
threshold production of energetic particles;
(vi) Interaction of neutrinos with nuclei;
(vii) The EMC effect.
A schematic illustration of these interactions is shown in figures 1 and 2.
2.1. Interaction of energetic photons (Eγ>40 MeV) with nuclei
In photoemission reactions, the outgoing nucleons were expected to follow either the di-
rect photoelectric process developed by Courant [7] in which photon energy is absorbed
by individual proton leading to its ejection from nucleus, or the statistical theory of
Blatt and Weisskopf [31] in which nucleons are assumed to “boil off” from the excited
compound system. However, it rapidly became apparent that the photo-neutron and
photo-proton production cross sections, and their ratio, could not be accounted for by ei-
ther of these reaction models. It became possible to investigate the photo-disintegration
of nuclei with much higher photon energies with the advent of bremsstrahlung photons
from synchrotrons. It was expected that only nucleonic degrees of freedom would be
important for Eγ100 MeV, and the (γ, p) reaction would be much more probable due
to its strong electric dipole component. In comparison the (γ, n) reaction has a much
weaker magnetic dipole contribution. Furthermore, no significant angular correlations
were expected between ejected nucleons for reactions in which more than one nucleon
were “boiled off”. However, energetic gamma-ray interactions resulted in comparable
σ(γ,n)and σ(γ,p)cross-section values which were much higher than the single particle
cross sections expected from Courant’s work.
Nucleon-Nucleon correlations inside atomic nuclei 5
Figure 1. Direct demonstration of strongly-correlated 2N clusters (mainly in form of
n-p pairs) by different incident particles.
Figure 2. Other direct and indirect manifestations of strongly-correlated 2N systems
inside nuclei.
摘要:

Nucleon-nucleoncorrelationsinsideatomicnuclei:synergies,observationsandtheoreticalmodelsRanjeetDalal1,andI.J.DouglasMacGregor21GuruJambheshwarUniversityofScienceandtechnology,Hisar,India2SUPASchoolofPhysicsandAstronomy,UniversityofGlasgow,GlasgowG128QQ,UnitedKingdomE-mail:ranjeet@gjust.orgAugust2022...

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