Schwinger effect

In the presence of a strong, constant electric field, electrons, e, and positrons, e+, will be spontaneously created.

The Schwinger effect is a predicted physical phenomenon whereby matter is created by a strong electric field. It is also referred to as the Sauter–Schwinger effect, Schwinger mechanism, or Schwinger pair production. It is a prediction of quantum electrodynamics (QED) in which electronpositron pairs are spontaneously created in the presence of an electric field, thereby causing the decay of the electric field. The effect was originally proposed by Fritz Sauter in 1931[1] and further important work was carried out by Werner Heisenberg and Hans Heinrich Euler in 1936,[2] though it was not until 1951 that Julian Schwinger gave a complete theoretical description.[3]

The Schwinger effect can be thought of as vacuum decay in the presence of an electric field. Although the notion of vacuum decay suggests that something is created out of nothing, physical conservation laws are nevertheless obeyed. To understand this, note that electrons and positrons are each other's antiparticles, with identical properties except opposite electric charge.

To conserve energy, the electric field loses energy when an electron–positron pair is created, by an amount equal to , where is the electron rest mass and is the speed of light. Electric charge is conserved because an electron–positron pair is charge neutral. Linear and angular momentum are conserved because, in each pair, the electron and positron are created with opposite velocities and spins. In fact, the electron and positron are expected to be created at (close to) rest, and then subsequently accelerated away from each other by the electric field.[4]

  1. ^ Sauter, Fritz (1931). "Über das Verhalten eines Elektrons im homogenen elektrischen Feld nach der relativistischen Theorie Diracs". Zeitschrift für Physik (in German). 69 (11–12). Springer Science and Business Media LLC: 742–764. Bibcode:1931ZPhy...69..742S. doi:10.1007/bf01339461. ISSN 1434-6001. S2CID 122120733.
  2. ^ Heisenberg, W.; Euler, H. (1936). "Folgerungen aus der Diracschen Theorie des Positrons". Zeitschrift für Physik (in German). 98 (11–12): 714–732. arXiv:physics/0605038. Bibcode:1936ZPhy...98..714H. doi:10.1007/bf01343663. ISSN 1434-6001.
  3. ^ Schwinger, Julian (1951-06-01). "On Gauge Invariance and Vacuum Polarization". Physical Review. 82 (5). American Physical Society (APS): 664–679. Bibcode:1951PhRv...82..664S. doi:10.1103/physrev.82.664. ISSN 0031-899X.
  4. ^ A.I. Nikishov (1970). "Pair Production by a Constant External Field". Journal of Experimental and Theoretical Physics. 30: 660.