Local theory

In physics, the principle of locality states that an object is influenced directly only by its immediate surroundings. A theory that includes the principle of locality is said to be a "local theory". This is an alternative to the concept of instantaneous " action at a distance". Locality evolved out of the field theories of classical physics. The concept is that for an action at one point to have an influence at another point, something in the space between those points must mediate the action. To exert an influence, something, such as a wave or particle, must travel through the space between the two points, carrying the influence.

The special theory of relativity limits the speed at which all such influences can travel to the speed of light, $c$. Therefore, the principle of locality implies that an event at one point cannot cause a simultaneous result at another point. An event at point $A$ cannot cause a result at point $B$ in a time less than $T=D/c$, where $D$ is the distance between the points and $c$ is the speed of light in a vacuum.

Experimental tests show that quantum mechanics seems to violate Bell's inequalities, implying that quantum effects might be non-local, according to some interpretations of quantum mechanics.

Pre-quantum mechanics

During the 17th century Newton's principle of universal gravitation was formulated in terms of "action at a distance", thereby violating the principle of locality.

Coulomb's law of electric forces was initially also formulated as instantaneous action at a distance, but was later superseded by Maxwell's equations of electromagnetism, which obey locality.

In 1905 Albert Einstein's special theory of relativity postulated that no material or energy can travel faster than the speed of light, and Einstein thereby sought to reformulate physics in a way that obeyed the principle of locality. He later succeeded in producing an alternative theory of gravitation, general relativity, which obeys the principle of locality.

However, a different challenge to the principle of locality developed subsequently from the theory of quantum mechanics, which Einstein himself had helped to create.

Quantum mechanics

Local realism

In 1935, Albert Einstein, Boris Podolsky and Nathan Rosen in their EPR paradox theorised that quantum mechanics might not be a local theory, because a measurement made on one of a pair of separated but '' entangled'' particles causes a ''simultaneous'' effect, the collapse of the wave function, in the remote particle (i.e., an effect exceeding the speed of light). But because of the probabilistic nature of wave function collapse, this violation of locality cannot be used to transmit information faster than light. In 1964 John Stewart Bell formulated the " Bell inequality", which, if violated in actual experiments, implies that quantum mechanics violates either locality or realism, another principle, which relates to the value of unmeasured quantities ( counterfactual definiteness). The two principles are commonly referred to as a single principle, local realism.

Experimental tests of the Bell inequality, beginning with John Clauser and Alain Aspect's 1980s experiments, show that quantum mechanics seems to violate the inequality, so it must violate either locality or realism. However, critics have noted these experiments included "loopholes", which prevented a definitive answer to this question. This problem is considered to have been resolved during 2015 when three "loophole-free" experiments were carried out In 2015 by independent groups in Delft University of Technology, University of Vienna and National Institute of Standards and Technology (NIST), addressing multiple loopholes at the same time. However, some loopholes might persist, like superdeterminism, with the result that the question may be fundamentally untestable.

Relativistic quantum mechanics

Locality is one of the axioms of relativistic quantum field theory, as required for causality. The formalization of locality in this case is as follows: if there are two observables, each localized within two distinct spacetime regions which happen to be at a spacelike separation from each other, the observables must commute. Alternatively, a solution to the field equations is local if the underlying equations are either Lorentz invariant or, more generally, generally covariant or locally Lorentz invariant.

See also

* Einstein's thought experiments
* Local hidden-variable theory
* Non-locality (disambiguation)
* Quantum nonlocality
* Cluster decomposition

References

External links

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Quantum nonlocality vs. Einstein locality
by H. Dieter Zeh

Quantum measurement