Investigation of charge symmetry violation in the mirror reactions 2H(d, p)3H and 2H(d, n)3He
References (19)
- et al.
Nucl. Phys.
(1972) - et al.
Nucl. Phys.
(1972) - et al.
Phys. Lett.
(1978) - et al.
Phys. Lett.
(1979) - et al.
Nucl. Phys.
(1969) - et al.
Nucl. Phys.
(1976) - et al.
Nucl. Phys.
(1972) - et al.
Cited by (20)
Differential and total cross sections and astrophysical S-factors for <sup>2</sup>H(d,n)<sup>3</sup>He and <sup>2</sup>H(d,p)<sup>3</sup>H reactions in a wide energy range
2018, Atomic Data and Nuclear Data TablesCitation Excerpt :Regarding the question of charge symmetry, its violations are known to be due to the perturbing effects of the mass difference between up and down quarks and electromagnetic interactions between the quarks [12]. Charge symmetry violation in reactions 2H(d,n)3He and 2H(d,p)3H was addressed in [13,14] and more recently in Ref. [15]. Calculations of nuclear fusion reaction rates, together with energetic and angular distributions of the products of these reactions, are an essential part of the physics basis for the ongoing work on neutron sources, demonstration power plant concepts and fusion–fission hybrid systems based on magnetic plasma confinement [16,17], for the development of blankets of such systems [18–20], and for the advancement of nuclear technologies of the controlled fusion [21–23].
Deuteron-deuteron scattering above four-nucleon breakup threshold
2015, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsCharge symmetry, quarks and mesons
1990, Physics ReportsNew polarization measurements in few-nucleon systems
1987, Nuclear Physics, Section AThe analyzing power for the <sup>2</sup>H(d, n)<sup>3</sup>He<inf>g.s.</inf> reaction from 5.5 to 11.5 MeV
1983, Nuclear Physics, Section A
- †
On leave from the Los Alamos Scientific Laboratory, Los Alamos, New Mexico 87545, USA.