Invariant differential yields of deuterons and antideuterons in pp collisions at s= 0.9, 2.76
and 7 TeV and the yields of tritons, He 3 nuclei, and their antinuclei at s= 7 TeV have been …

Nuclear collisions recreate conditions in the universe microseconds after the Big Bang. Only
a very small fraction of the emitted fragments are light nuclei, but these states are of …

The measurement of the production of deuterons, tritons and He 3 and their antiparticles in
Pb-Pb collisions at s NN= 5.02 TeV is presented in this article. The measurements are …

A microscopic understanding of (anti) deuteron production in hadron–hadron collisions is
the subject of many experimental and theoretical efforts in nuclear physics. This topic is also …

A bstract Understanding the production mechanism of light (anti) nuclei is one of the key
challenges of nuclear physics and has important consequences for astrophysics, since it …

In our Galaxy, light antinuclei composed of antiprotons and antineutrons can be produced
through high-energy cosmic-ray collisions with the interstellar medium or could also …

In this Letter, we report the first measurement of the inelastic cross section for antideuteron-
nucleus interactions at low particle momenta, covering a range of 0.3≤ p< 4 GeV/c. The …

Deuteron and anti-deuteron production in Z decays has been observed in the ALEPH
experiment at LEP. The production rate of anti-deuterons is measured to be (5.9±1.8±0.5)× …

Abstract Measurements of (anti) proton,(anti) deuteron, and (anti) 3 He production in the
rapidity range− 1< y< 0 as a function of the transverse momentum and event multiplicity in p …

The energy dependence of light (anti) nuclei and (anti) hypertriton production are
investigated in central Au-Au collisions from AGS up to LHC energies at midrapidity, using …