
Symmetry of physical laws under reversal of time; its breaking enables certain transport effects.Time reversal symmetry is the principle that the fundamental laws of physics remain valid if the direction of time is reversed. In equations, this means that if a process is physically allowed, then the exact reverse process, with all velocities and momenta flipped, is also allowed. This symmetry holds for the strong, weak, and electromagnetic forces under specific conditions, and it underpins the idea that at the microscopic level, physical processes are reversible — they look the same whether played forward or backward.
The concept was formalized in the 1930s by Eugene Wigner, who introduced the anti-unitary time reversal operator in quantum mechanics. The possibility of its violation in the weak interaction was proposed by Lev Landau in 1957, following the discovery of parity violation.
In quantum mechanics, time reversal symmetry is implemented by an anti-unitary operator that flips the sign of time, momentum, and angular momentum. For a system to respect this symmetry, its Hamiltonian must commute with this operator. When this symmetry is unbroken, certain transport coefficients, like electrical conductivity, obey Onsager relations that link forward and reverse processes. Breaking this symmetry — for example, by applying a magnetic field or through the weak interaction — allows for phenomena like the Hall effect, where currents flow perpendicular to an applied electric field, and other one-way transport effects.
Time reversal symmetry breaking is exploited in spintronics and topological insulators, where it enables the robust, dissipationless transport of spin or charge, and in the design of magnetic memory devices.
The violation of time reversal symmetry in the weak force is one of the necessary conditions for the observed matter-antimatter asymmetry in the universe, as it allows processes that distinguish between forward and backward time.






