Nonlocal single particle steering generated through single particle entanglement
Abstract In 1927, at the Solvay conference, Einstein posed a thought experiment with the primary intention of showing the incompleteness of quantum mechanics; to prove it, he employed the instantaneous nonlocal effects caused by the collapse of the wavefunction of a single particle—the spooky action...
Main Author: | |
---|---|
Format: | Article |
Language: | English |
Published: |
Nature Publishing Group
2021-03-01
|
Series: | Scientific Reports |
Online Access: | https://doi.org/10.1038/s41598-021-85508-8 |
id |
doaj-4666d609adda4fdf8e5a8de6fd56528e |
---|---|
record_format |
Article |
spelling |
doaj-4666d609adda4fdf8e5a8de6fd56528e2021-03-28T11:29:01ZengNature Publishing GroupScientific Reports2045-23222021-03-0111111110.1038/s41598-021-85508-8Nonlocal single particle steering generated through single particle entanglementL. M. Arévalo Aguilar0Facultad de Ciencias Físico Matemáticas, Benemérita Universidad Autónoma de PueblaAbstract In 1927, at the Solvay conference, Einstein posed a thought experiment with the primary intention of showing the incompleteness of quantum mechanics; to prove it, he employed the instantaneous nonlocal effects caused by the collapse of the wavefunction of a single particle—the spooky action at a distance–, when a measurement is done. This historical event preceded the well-know Einstein–Podolsk–Rosen criticism over the incompleteness of quantum mechanics. Here, by using the Stern–Gerlach experiment, we demonstrate how the instantaneous nonlocal feature of the collapse of the wavefunction together with the single-particle entanglement can be used to produce the nonlocal effect of steering, i.e. the single-particle steering. In the steering process Bob gets a quantum state depending on which observable Alice decides to measure. To accomplish this, we fully exploit the spreading (over large distances) of the entangled wavefunction of the single-particle. In particular, we demonstrate that the nonlocality of the single-particle entangled state allows the particle to “know” about the kind of detector Alice is using to steer Bob’s state. Therefore, notwithstanding strong counterarguments, we prove that the single-particle entanglement gives rise to truly nonlocal effects at two faraway places. This opens the possibility of using the single-particle entanglement for implementing truly nonlocal task.https://doi.org/10.1038/s41598-021-85508-8 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
L. M. Arévalo Aguilar |
spellingShingle |
L. M. Arévalo Aguilar Nonlocal single particle steering generated through single particle entanglement Scientific Reports |
author_facet |
L. M. Arévalo Aguilar |
author_sort |
L. M. Arévalo Aguilar |
title |
Nonlocal single particle steering generated through single particle entanglement |
title_short |
Nonlocal single particle steering generated through single particle entanglement |
title_full |
Nonlocal single particle steering generated through single particle entanglement |
title_fullStr |
Nonlocal single particle steering generated through single particle entanglement |
title_full_unstemmed |
Nonlocal single particle steering generated through single particle entanglement |
title_sort |
nonlocal single particle steering generated through single particle entanglement |
publisher |
Nature Publishing Group |
series |
Scientific Reports |
issn |
2045-2322 |
publishDate |
2021-03-01 |
description |
Abstract In 1927, at the Solvay conference, Einstein posed a thought experiment with the primary intention of showing the incompleteness of quantum mechanics; to prove it, he employed the instantaneous nonlocal effects caused by the collapse of the wavefunction of a single particle—the spooky action at a distance–, when a measurement is done. This historical event preceded the well-know Einstein–Podolsk–Rosen criticism over the incompleteness of quantum mechanics. Here, by using the Stern–Gerlach experiment, we demonstrate how the instantaneous nonlocal feature of the collapse of the wavefunction together with the single-particle entanglement can be used to produce the nonlocal effect of steering, i.e. the single-particle steering. In the steering process Bob gets a quantum state depending on which observable Alice decides to measure. To accomplish this, we fully exploit the spreading (over large distances) of the entangled wavefunction of the single-particle. In particular, we demonstrate that the nonlocality of the single-particle entangled state allows the particle to “know” about the kind of detector Alice is using to steer Bob’s state. Therefore, notwithstanding strong counterarguments, we prove that the single-particle entanglement gives rise to truly nonlocal effects at two faraway places. This opens the possibility of using the single-particle entanglement for implementing truly nonlocal task. |
url |
https://doi.org/10.1038/s41598-021-85508-8 |
work_keys_str_mv |
AT lmarevaloaguilar nonlocalsingleparticlesteeringgeneratedthroughsingleparticleentanglement |
_version_ |
1724199963746893824 |