Matches in SemOpenAlex for { <https://semopenalex.org/work/W3214995042> ?p ?o ?g. }
- W3214995042 endingPage "127849" @default.
- W3214995042 startingPage "127849" @default.
- W3214995042 abstract "• Quantum measurements. • Back action and Standard Quantum Limit. • Back action evading. • Variational measurement: narrow band back action evading. • Dichromatic variational measurement: broad band back action evading. Quantum back action imposes fundamental sensitivity limits to the majority of quantum measurements. The effect results from the unavoidable contamination of the measured parameter with the quantum noise of a meter. Back action evading measurements take advantage of the quantum correlations introduced by the system under study to the meter and allow overcoming the fundamental limitations. The measurements are frequently restricted in their bandwidth due to a finite response time of the system components. Here we show that probing a mechanical oscillator with a dichromatic field with frequencies separated by the oscillator frequency enables independent detection in two outputs and complete subtraction of the measurement noise associated with the quantum back action." @default.
- W3214995042 created "2021-12-06" @default.
- W3214995042 creator A5019420372 @default.
- W3214995042 creator A5086080860 @default.
- W3214995042 date "2022-02-01" @default.
- W3214995042 modified "2023-10-03" @default.
- W3214995042 title "Broadband quantum back action evading measurements of a resonant force" @default.
- W3214995042 cites W1968415019 @default.
- W3214995042 cites W1969658805 @default.
- W3214995042 cites W1983329723 @default.
- W3214995042 cites W1995571734 @default.
- W3214995042 cites W2005208156 @default.
- W3214995042 cites W2006041002 @default.
- W3214995042 cites W2038674186 @default.
- W3214995042 cites W2045275528 @default.
- W3214995042 cites W2052668135 @default.
- W3214995042 cites W2064221608 @default.
- W3214995042 cites W2072837367 @default.
- W3214995042 cites W2075537159 @default.
- W3214995042 cites W2076253155 @default.
- W3214995042 cites W2093188166 @default.
- W3214995042 cites W2095619950 @default.
- W3214995042 cites W2103682879 @default.
- W3214995042 cites W2122233615 @default.
- W3214995042 cites W2127113568 @default.
- W3214995042 cites W2127965801 @default.
- W3214995042 cites W2128938328 @default.
- W3214995042 cites W2139031855 @default.
- W3214995042 cites W2158293236 @default.
- W3214995042 cites W2170552223 @default.
- W3214995042 cites W2272565422 @default.
- W3214995042 cites W2332198693 @default.
- W3214995042 cites W2515386134 @default.
- W3214995042 cites W2613794917 @default.
- W3214995042 cites W2781060599 @default.
- W3214995042 cites W2885965202 @default.
- W3214995042 cites W2892360226 @default.
- W3214995042 cites W2923360235 @default.
- W3214995042 cites W2977312509 @default.
- W3214995042 cites W2979401873 @default.
- W3214995042 cites W2993051973 @default.
- W3214995042 cites W2999458734 @default.
- W3214995042 cites W3015534879 @default.
- W3214995042 cites W3037306418 @default.
- W3214995042 cites W3103449652 @default.
- W3214995042 cites W3122448994 @default.
- W3214995042 cites W3124044376 @default.
- W3214995042 cites W4247044223 @default.
- W3214995042 cites W930220367 @default.
- W3214995042 doi "https://doi.org/10.1016/j.physleta.2021.127849" @default.
- W3214995042 hasPublicationYear "2022" @default.
- W3214995042 type Work @default.
- W3214995042 sameAs 3214995042 @default.
- W3214995042 citedByCount "0" @default.
- W3214995042 crossrefType "journal-article" @default.
- W3214995042 hasAuthorship W3214995042A5019420372 @default.
- W3214995042 hasAuthorship W3214995042A5086080860 @default.
- W3214995042 hasBestOaLocation W32149950421 @default.
- W3214995042 hasConcept C115961682 @default.
- W3214995042 hasConcept C120665830 @default.
- W3214995042 hasConcept C121332964 @default.
- W3214995042 hasConcept C154945302 @default.
- W3214995042 hasConcept C180214583 @default.
- W3214995042 hasConcept C2780791683 @default.
- W3214995042 hasConcept C3079626 @default.
- W3214995042 hasConcept C41008148 @default.
- W3214995042 hasConcept C509933004 @default.
- W3214995042 hasConcept C62520636 @default.
- W3214995042 hasConcept C74650414 @default.
- W3214995042 hasConcept C84114770 @default.
- W3214995042 hasConcept C99498987 @default.
- W3214995042 hasConceptScore W3214995042C115961682 @default.
- W3214995042 hasConceptScore W3214995042C120665830 @default.
- W3214995042 hasConceptScore W3214995042C121332964 @default.
- W3214995042 hasConceptScore W3214995042C154945302 @default.
- W3214995042 hasConceptScore W3214995042C180214583 @default.
- W3214995042 hasConceptScore W3214995042C2780791683 @default.
- W3214995042 hasConceptScore W3214995042C3079626 @default.
- W3214995042 hasConceptScore W3214995042C41008148 @default.
- W3214995042 hasConceptScore W3214995042C509933004 @default.
- W3214995042 hasConceptScore W3214995042C62520636 @default.
- W3214995042 hasConceptScore W3214995042C74650414 @default.
- W3214995042 hasConceptScore W3214995042C84114770 @default.
- W3214995042 hasConceptScore W3214995042C99498987 @default.
- W3214995042 hasFunder F4320306101 @default.
- W3214995042 hasFunder F4320321079 @default.
- W3214995042 hasLocation W32149950421 @default.
- W3214995042 hasOpenAccess W3214995042 @default.
- W3214995042 hasPrimaryLocation W32149950421 @default.
- W3214995042 hasRelatedWork W1570413653 @default.
- W3214995042 hasRelatedWork W1619281770 @default.
- W3214995042 hasRelatedWork W1977012935 @default.
- W3214995042 hasRelatedWork W2008049436 @default.
- W3214995042 hasRelatedWork W2054061985 @default.
- W3214995042 hasRelatedWork W2073594599 @default.
- W3214995042 hasRelatedWork W2078124205 @default.
- W3214995042 hasRelatedWork W2120793651 @default.
- W3214995042 hasRelatedWork W2400054357 @default.