Can single photon excitation of two spatially separated modes lead to a violation of Bell inequality via weak-field homodyne measurements?
We reconsider the all-optical weak homodyne-measurement based experimental schemes aimed at revealing Bell nonclassicality (‘nonlocality’) of a single photon. We focus on the schemes put forward by Tan et al (TWC, 1991) and Hardy (1994). In our previous work we show that the TWC experiment can be de...
| Published in: | New Journal of Physics |
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| Main Authors: | , , , , , |
| Format: | Article |
| Language: | English |
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IOP Publishing
2021-01-01
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| Online Access: | https://doi.org/10.1088/1367-2630/ac0ffe |
| _version_ | 1851950892014632960 |
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| author | Tamoghna Das Marcin Karczewski Antonio Mandarino Marcin Markiewicz Bianka Woloncewicz Marek Żukowski |
| author_facet | Tamoghna Das Marcin Karczewski Antonio Mandarino Marcin Markiewicz Bianka Woloncewicz Marek Żukowski |
| author_sort | Tamoghna Das |
| collection | DOAJ |
| container_title | New Journal of Physics |
| description | We reconsider the all-optical weak homodyne-measurement based experimental schemes aimed at revealing Bell nonclassicality (‘nonlocality’) of a single photon. We focus on the schemes put forward by Tan et al (TWC, 1991) and Hardy (1994). In our previous work we show that the TWC experiment can be described by a local hidden variable model, hence the claimed nonclassicality is apparent. The nonclassicality proof proposed by Hardy remains impeccable. We investigate which feature of the Hardy’s approach is crucial to disclose the nonclassicality. There are consequential differences between TWC and Hardy setups: (i) the initial state of Hardy is a superposition of a single photon excitation with vacuum in one of the input modes of a 50–50 beamsplitter. In the TWC case there is no vacuum component. (ii) In the final measurements of Hardy’s proposal the local settings are specified by the presence or absence of a local oscillator field (on/off). In the TWC case the auxiliary fields are constant, only phases are varied. We show that in Hardy’s setup the violation of local realism occurs due to the varying strength of the local oscillators. Still, one does not need to operate in the fully on/off detection scheme. Thus, the nonclassicality in a Hardy-like setup cannot be attributed to the single-photon state alone. It is a consequence of its interference with the photons from auxiliary local fields. Neither can it be attributed to the joint state of the single photon excitation and the local oscillator modes, as this state is measurement setting dependent. Despite giving spurious violations of local realism, the TWC scheme can serve as an entanglement indicator, for the TWC state. Nevertheless an analogue indicator based on intensity rates rather than just intensities overperforms it. |
| format | Article |
| id | doaj-art-e014ba14c3bb4e76a59a21ebceef5e56 |
| institution | Directory of Open Access Journals |
| issn | 1367-2630 |
| language | English |
| publishDate | 2021-01-01 |
| publisher | IOP Publishing |
| record_format | Article |
| spelling | doaj-art-e014ba14c3bb4e76a59a21ebceef5e562025-08-19T21:46:37ZengIOP PublishingNew Journal of Physics1367-26302021-01-0123707304210.1088/1367-2630/ac0ffeCan single photon excitation of two spatially separated modes lead to a violation of Bell inequality via weak-field homodyne measurements?Tamoghna Das0https://orcid.org/0000-0002-8074-6720Marcin Karczewski1https://orcid.org/0000-0002-9120-3377Antonio Mandarino2https://orcid.org/0000-0003-3745-5204Marcin Markiewicz3https://orcid.org/0000-0002-8983-9077Bianka Woloncewicz4https://orcid.org/0000-0002-4039-9146Marek Żukowski5https://orcid.org/0000-0001-7882-7962International Centre for Theory of Quantum Technologies, University of Gdańsk , 80-308 Gdańsk, PolandInternational Centre for Theory of Quantum Technologies, University of Gdańsk , 80-308 Gdańsk, PolandInternational Centre for Theory of Quantum Technologies, University of Gdańsk , 80-308 Gdańsk, PolandInternational Centre for Theory of Quantum Technologies, University of Gdańsk , 80-308 Gdańsk, PolandInternational Centre for Theory of Quantum Technologies, University of Gdańsk , 80-308 Gdańsk, PolandInternational Centre for Theory of Quantum Technologies, University of Gdańsk , 80-308 Gdańsk, PolandWe reconsider the all-optical weak homodyne-measurement based experimental schemes aimed at revealing Bell nonclassicality (‘nonlocality’) of a single photon. We focus on the schemes put forward by Tan et al (TWC, 1991) and Hardy (1994). In our previous work we show that the TWC experiment can be described by a local hidden variable model, hence the claimed nonclassicality is apparent. The nonclassicality proof proposed by Hardy remains impeccable. We investigate which feature of the Hardy’s approach is crucial to disclose the nonclassicality. There are consequential differences between TWC and Hardy setups: (i) the initial state of Hardy is a superposition of a single photon excitation with vacuum in one of the input modes of a 50–50 beamsplitter. In the TWC case there is no vacuum component. (ii) In the final measurements of Hardy’s proposal the local settings are specified by the presence or absence of a local oscillator field (on/off). In the TWC case the auxiliary fields are constant, only phases are varied. We show that in Hardy’s setup the violation of local realism occurs due to the varying strength of the local oscillators. Still, one does not need to operate in the fully on/off detection scheme. Thus, the nonclassicality in a Hardy-like setup cannot be attributed to the single-photon state alone. It is a consequence of its interference with the photons from auxiliary local fields. Neither can it be attributed to the joint state of the single photon excitation and the local oscillator modes, as this state is measurement setting dependent. Despite giving spurious violations of local realism, the TWC scheme can serve as an entanglement indicator, for the TWC state. Nevertheless an analogue indicator based on intensity rates rather than just intensities overperforms it.https://doi.org/10.1088/1367-2630/ac0ffenonclassicality of single photon excitationBell inequalitieshomodyne measurementmode entanglemententanglement witnessoperators based on rates |
| spellingShingle | Tamoghna Das Marcin Karczewski Antonio Mandarino Marcin Markiewicz Bianka Woloncewicz Marek Żukowski Can single photon excitation of two spatially separated modes lead to a violation of Bell inequality via weak-field homodyne measurements? nonclassicality of single photon excitation Bell inequalities homodyne measurement mode entanglement entanglement witness operators based on rates |
| title | Can single photon excitation of two spatially separated modes lead to a violation of Bell inequality via weak-field homodyne measurements? |
| title_full | Can single photon excitation of two spatially separated modes lead to a violation of Bell inequality via weak-field homodyne measurements? |
| title_fullStr | Can single photon excitation of two spatially separated modes lead to a violation of Bell inequality via weak-field homodyne measurements? |
| title_full_unstemmed | Can single photon excitation of two spatially separated modes lead to a violation of Bell inequality via weak-field homodyne measurements? |
| title_short | Can single photon excitation of two spatially separated modes lead to a violation of Bell inequality via weak-field homodyne measurements? |
| title_sort | can single photon excitation of two spatially separated modes lead to a violation of bell inequality via weak field homodyne measurements |
| topic | nonclassicality of single photon excitation Bell inequalities homodyne measurement mode entanglement entanglement witness operators based on rates |
| url | https://doi.org/10.1088/1367-2630/ac0ffe |
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