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Diffraction in time : ウィキペディア英語版
Diffraction in time
Diffraction in time is a phenomenon associated with the quantum dynamics of suddenly released matter waves initially confined in a region of space.
It was introduced in 1952 by Marcos Moshinsky with the ''shutter problem''
:〔
〕 A matter-wave beam stopped by an absorbing shutter exhibits an oscillatory density profile during its propagation after removal of the shutter. Whenever this propagation is accurately described by the time-dependent Schrödinger equation, the transient wave functions resemble the solutions that appear for the intensity of light subject to Fresnel diffraction by a straight edge. For this reason, the transient phenomenon was dubbed diffraction in time and has since then been recognised as ubiquitous in quantum dynamics.




The experimental confirmation of this phenomenon was only achieved about half a century later in the group of ultracold atoms directed by Jean Dalibard.〔

== References ==


抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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