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In
nuclear physics Nuclear physics is the field of physics that studies atomic nuclei and their constituents and interactions, in addition to the study of other forms of nuclear matter. Nuclear physics should not be confused with atomic physics, which studies th ...
, an
atomic nucleus The atomic nucleus is the small, dense region consisting of protons and neutrons at the center of an atom, discovered in 1911 by Ernest Rutherford at the Department_of_Physics_and_Astronomy,_University_of_Manchester , University of Manchester ...
is called a halo nucleus or is said to have a nuclear halo when it has a core nucleus surrounded by a "halo" of orbiting protons or neutrons, which makes the radius of the nucleus appreciably larger than that predicted by the liquid drop model. Halo nuclei form at the extreme edges of the table of nuclides — the
neutron drip line The nuclear drip line is the boundary beyond which atomic nuclei are unbound with respect to the emission of a proton or neutron. An arbitrary combination of protons and neutrons does not necessarily yield a stable nucleus. One can think of m ...
and
proton drip line The nuclear drip line is the boundary beyond which atomic nuclei are unbound with respect to the emission of a proton or neutron. An arbitrary combination of protons and neutrons does not necessarily yield a stable nucleus. One can think of m ...
— and have short half-lives, measured in milliseconds. These nuclei are studied shortly after their formation in an
ion beam An ion beam is a beam of ions, a type of charged particle beam. Ion beams have many uses in electronics manufacturing (principally ion implantation) and other industries. There are many ion beam sources, some derived from the mercury vapor ...
. Typically, an atomic nucleus is a tightly bound group of protons and neutrons. However, in some nuclides, there is an overabundance of one species of nucleon. In some of these cases, a nuclear core and a halo will form. Often, this property may be detected in scattering experiments, which show the nucleus to be much larger than the otherwise expected value. Normally, the cross-section (corresponding to the classical radius) of the nucleus is proportional to the cube root of its mass, as would be the case for a sphere of constant density. Specifically, for a nucleus of
mass number The mass number (symbol ''A'', from the German word: ''Atomgewicht'', "atomic weight"), also called atomic mass number or nucleon number, is the total number of protons and neutrons (together known as nucleons) in an atomic nucleus. It is appro ...
''A'', the radius ''r'' is (approximately) :r = r_\circ A^, where r_\circ is 1.2 fm. One example of a halo nucleus is 11 Li, which has a half-life of 8.6 ms. It contains a core of 3 protons and 6 neutrons, and a halo of two independent and loosely bound neutrons. It decays into 11 Be by the emission of an antineutrino and an electron. Its mass radius of 3.16 fm is close to that of 32 S or, even more impressively, of 208 Pb, both much heavier nuclei. Experimental confirmation of nuclear halos is recent and ongoing. Additional candidates are suspected. Several nuclides including 9B, 13N, and 15N are calculated to have a halo in the
excited state In quantum mechanics Quantum mechanics is the fundamental physical Scientific theory, theory that describes the behavior of matter and of light; its unusual characteristics typically occur at and below the scale of atoms. Reprinted, Add ...
but not in the
ground state The ground state of a quantum-mechanical system is its stationary state of lowest energy; the energy of the ground state is known as the zero-point energy of the system. An excited state is any state with energy greater than the ground state ...
.


List of known nuclides with nuclear halo

Nuclei that have a neutron halo include 11 Be and 19 C. A two-neutron halo is exhibited by 6 He, 11 Li, 17 B, 19 B and 22 C. Two-neutron halo nuclei break into three fragments and are called Borromean because of this behavior, analogously to how all three of the
Borromean rings In mathematics, the Borromean rings are three simple closed curves in three-dimensional space that are link (knot theory), topologically linked and cannot be separated from each other, but that break apart into two unknotted and unlinked loops wh ...
are linked together but no two share a link. For example, the two-neutron halo nucleus 6He (which can be taken as a three-body system consisting of an alpha particle and two neutrons) is bound, but neither 5He nor the dineutron is. 8 He and 14 Be both exhibit a four-neutron halo. Nuclei that have a proton halo include 8 B and 26 P. A two-proton halo is exhibited by 17 Ne and 27 S. Proton halos are expected to be rarer and more unstable than neutron halos because of the repulsive forces of the excess proton(s).


See also

* Halo nuclei and nuclear force range limits * Isotopes of lithium *
Exotic atom An exotic atom is an otherwise normal atom in which one or more sub-atomic particles have been replaced by other particles. For example, electrons may be replaced by other negatively charged particles such as muons (muonic atoms) or pions (pionic a ...
* Borromean nucleus


References


Further reading

* * *{{cite journal , arxiv=nucl-ex/0111001 , doi=10.1103/PhysRevC.65.044006 , title=Detection of neutron clusters , year=2002 , last1=Marqués , first1=F. M. , last2=Labiche , first2=M. , last3=Orr , first3=N. A. , last4=Angélique , first4=J. C. , last5=Axelsson , first5=L. , last6=Benoit , first6=B. , last7=Bergmann , first7=U. C. , last8=Borge , first8=M. J. G. , last9=Catford , first9=W. N. , last10=Chappell , first10=S. P. G. , last11=Clarke , first11=N. M. , last12=Costa , first12=G. , last13=Curtis , first13=N. , last14=d'Arrigo , first14=A. , last15=De Góes Brennand , first15=E. , last16=De Oliveira Santos , first16=F. , last17=Dorvaux , first17=O. , last18=Fazio , first18=G. , last19=Freer , first19=M. , last20=Fulton , first20=B. R. , last21=Giardina , first21=G. , last22=Grévy , first22=S. , last23=Guillemaud-Mueller , first23=D. , last24=Hanappe , first24=F. , last25=Heusch , first25=B. , last26=Jonson , first26=B. , last27=Le Brun , first27=C. , last28=Leenhardt , first28=S. , last29=Lewitowicz , first29=M. , last30=López , first30=M. J. , s2cid=37431352 , journal=Physical Review C , volume=65 , issue=4 , page=044006 , bibcode=2002PhRvC..65d4006M , display-authors=29 Nuclear physics