Abstract:A superstrong magnetic field stimulates the spontaneous production of positrons by naked nuclei by diminishing the value of the critical charge Z cr . The phenomenon of screening of the Coulomb potential by a superstrong magnetic field which has been discovered recently acts in the opposite direction and prevents the nuclei with Z < 52 from becoming critical. For Z > 52 for a nucleus to become critical stronger B are needed than without taking screening into account.
“…The details of this calculation can be found in [12]. The results for ground energy level for the ion with Z = 40 are presented in Table 1.…”
Section: Critical Nucleus Charge In the Modified Potentialmentioning
confidence: 99%
“…With the help of this formula the potential for 2 z = 0 with arbitrary ρ and for ρ = 0 with arbitrary z was calculated analytically [11,12]. It was found [7,8,12] that for z 1/m the equipotential lines are ellipses, though the potential in the mid-range distances, r = ρ 2 + z 2 1/m, was still unknown. In Fig.…”
Section: Epj Web Of Conferences 182mentioning
confidence: 99%
“…Using formula (5) the analytical expressions for Φ (0, z) and Φ (ρ, 0) were found [11,12] (see also asymptotics in [7,8]):…”
Section: Modification Of the Coulomb Potential By External Superstronmentioning
Abstract. Due to strong enhancement of loop effects in a superstrong magnetic field (B m 2 /e 3 ) the Coulomb potential becomes screened. This phenomenon dramatically changes the dependence of the electron energy levels on magnetic field. In particular, the freezing of energy levels occurs so the ground energy level of light ions can never reach the lower continuum (become critical), no matter how strong the field is. Therefore, the magnetic field affects the critical nucleus charge Z cr in two ways: i. it makes the electron movement essentially one-dimensional diminishing the value of Z cr ; ii. it makes the potential weaker increasing the value of critical charge. The phenomenon of critical charge itself is also discussed.
“…The details of this calculation can be found in [12]. The results for ground energy level for the ion with Z = 40 are presented in Table 1.…”
Section: Critical Nucleus Charge In the Modified Potentialmentioning
confidence: 99%
“…With the help of this formula the potential for 2 z = 0 with arbitrary ρ and for ρ = 0 with arbitrary z was calculated analytically [11,12]. It was found [7,8,12] that for z 1/m the equipotential lines are ellipses, though the potential in the mid-range distances, r = ρ 2 + z 2 1/m, was still unknown. In Fig.…”
Section: Epj Web Of Conferences 182mentioning
confidence: 99%
“…Using formula (5) the analytical expressions for Φ (0, z) and Φ (ρ, 0) were found [11,12] (see also asymptotics in [7,8]):…”
Section: Modification Of the Coulomb Potential By External Superstronmentioning
Abstract. Due to strong enhancement of loop effects in a superstrong magnetic field (B m 2 /e 3 ) the Coulomb potential becomes screened. This phenomenon dramatically changes the dependence of the electron energy levels on magnetic field. In particular, the freezing of energy levels occurs so the ground energy level of light ions can never reach the lower continuum (become critical), no matter how strong the field is. Therefore, the magnetic field affects the critical nucleus charge Z cr in two ways: i. it makes the electron movement essentially one-dimensional diminishing the value of Z cr ; ii. it makes the potential weaker increasing the value of critical charge. The phenomenon of critical charge itself is also discussed.
“…The role of screening of the Coulomb interaction in MF has a long story, see e.g. [8][9][10][11][12][13][14] for atomic systems.…”
Section: One-gluon Exchange In Mfmentioning
confidence: 99%
“…These topics are important in astrophysics of neutron stars [3][4][5][6], in cosmological theories [7], in atomic physics [8][9][10][11][12][13][14][15] in the physics of heavy ion collisions [16,17], and in the high-intensity lasers [18].…”
Spectra of qq hadrons are investigated in the framework of the Hamiltonian obtained from the relativistic path integral in external homogeneous magnetic field. The spectra of all 12 spin-isospin s-wave states, generated by π and ρ mesons with different spin projections, are studied both analytically and numerically on the lattice as functions of (magnetic field) eB. Results are in agreement and demonstrate three types of behavior, with characteristic splittings predicted by the theory.
Neutral systems containing two identical particles, in homogeneous magnetic field are shown to obey exact factorizable solutions both in nonrelativistic and relativistic formalism, similarly to the neutral twobody systems. Concrete examples of the helium atom and the neutron as a (ddu) system are considered.
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