Editing Quantum tunnelling (section)

== Related phenomena ==
Several phenomena have the same behavior as quantum tunnelling. Two examples are [[evanescent wave coupling]]<ref>{{Cite journal |last1=Martin |first1=Th. |last2=Landauer |first2=R. |date=1992-02-01 |title=Time delay of evanescent electromagnetic waves and the analogy to particle tunneling |url=https://link.aps.org/doi/10.1103/PhysRevA.45.2611 |journal=Physical Review A |language=en |volume=45 |issue=4 |pages=2611–2617 |doi=10.1103/PhysRevA.45.2611 |pmid=9907285 |bibcode=1992PhRvA..45.2611M |issn=1050-2947}}</ref> (the application of [[Maxwell's equations|Maxwell's wave-equation]] to [[light]]) and the application of the [[wave equation|non-dispersive wave-equation]] from [[acoustics]] applied to [[Wave#Waves on strings|"waves on strings"]].{{citation needed|date=April 2024}}

These effects are modeled similarly to the [[rectangular potential barrier]]. In these cases, one [[transmission medium]] through which the [[wave propagation|wave propagates]] that is the same or nearly the same throughout, and a second medium through which the wave travels differently. This can be described as a thin region of medium B between two regions of medium A. The analysis of a rectangular barrier by means of the Schrödinger equation can be adapted to these other effects provided that the wave equation has [[travelling wave]] solutions in medium A but real [[exponential function|exponential]] solutions in medium B.

In [[optics]], medium A is a vacuum while medium B is glass. In acoustics, medium A may be a liquid or gas and medium B a solid. For both cases, medium A is a region of space where the particle's [[total energy]] is greater than its [[potential energy]] and medium B is the potential barrier. These have an incoming wave and resultant waves in both directions. There can be more mediums and barriers, and the barriers need not be discrete. Approximations are useful in this case.

A classical wave-particle association was originally analyzed as analogous to quantum tunneling,<ref>{{cite journal|last1=Eddi|first1=A.|last2=Fort|first2=E.|last3=Moisy|first3=F.|last4=Couder|first4=Y.|title=Unpredictable Tunneling of a Classical Wave-Particle Association|journal=Physical Review Letters|date=16 June 2009|volume=102|issue=24|doi=10.1103/PhysRevLett.102.240401|url=http://stilton.tnw.utwente.nl/people/eddi/Papers/PhysRevLett_TUNNEL.pdf|access-date=1 May 2016|bibcode=2009PhRvL.102x0401E|pmid=19658983|page=240401|archive-date=10 March 2016|archive-url=https://web.archive.org/web/20160310083947/http://stilton.tnw.utwente.nl/people/eddi/Papers/PhysRevLett_TUNNEL.pdf|url-status=dead}}</ref> but subsequent analysis found a fluid dynamics cause related to the vertical momentum imparted to particles near the barrier.<ref>{{Cite journal |last1=Bush |first1=John W M |last2=Oza |first2=Anand U |date=2021-01-01 |title=Hydrodynamic quantum analogs |url=https://iopscience.iop.org/article/10.1088/1361-6633/abc22c |journal=Reports on Progress in Physics |volume=84 |issue=1 |pages=017001 |doi=10.1088/1361-6633/abc22c |pmid=33065567 |issn=0034-4885}}</ref>