The Schwinger effect is the creation of particle-antiparticle pairs from a vacuum by a strong electric field.Julian Schwinger, one of the creators of quantum electrodynamics, realized in 1951: if the electric field exceeds a fantastic value of about 10^18 V/m, the vacuum becomes unstable. Quantum fluctuations — virtual particle pairs — will be torn apart by the field and become real. Schwinger derived a formula showing that pair production is similar to tunneling: exponentially small in a weak field and catastrophically increasing at the critical value. This phenomenon is a close relative of Hawking radiation and particle production in the early Universe.
Julian Schwinger predicted the effect in 1951 in a paper on gauge invariance and vacuum polarization. Searches are being conducted in experiments with powerful lasers (SLAC, ELI) and at heavy ion colliders: in 2022, the STAR collaboration reported a possible observation of Schwinger breakdown in peripheral gold ion collisions, where fields briefly reached 10^20 V/m.
The effect occurs when the field work over the Compton wavelength of the electron exceeds 2m_e c^2. At E ~ E_c, vacuum polarization becomes nonlinear, and the back-reaction of the created particles must be taken into account. Reaching the critical field in the laboratory requires colossal intensity; schemes with next-generation colliders are promising. Astrophysical candidates are the vicinities of magnetars. In solid-state physics, an analogue is realized in Dirac materials (graphene) due to the small effective mass of charge carriers.
Direct observation requires fields billions of times stronger than laboratory ones, but in graphene, where the effective mass of electrons is small, it is possible to simulate a similar breakdown, promising a breakthrough in terahertz electronics.
Physicists hope to 'boil' the vacuum with next-generation X-ray lasers, and for now reproduce a mini-Schwinger in graphene, obtaining an avalanche of electrons and holes.
| v | variable | relative velocity of source and observer along the line of sight — velocity metre per second |
| Δλ | variable | observed wavelength shift (λ_observed - λ_0) — wavelength shift metre |
| λ_0 | variable | rest wavelength of the emitted light — wavelength metre |
| c | constant | speed of light in vacuum — speed of light = 299792458 metre per second |




















