FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W3135453966> ?p ?o ?g. }

• W3135453966 endingPage "063201" @default.
• W3135453966 startingPage "063201" @default.
• W3135453966 abstract "We present a high-sensitivity weak microwave measurement and communication technology by employing the Rydberg beat technique. The Rydberg cascade three-level system is composed of a cesium ground state <inline-formula><tex-math id=M8>begin{document}$6{rm{S}}_{1/2}$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M8.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M8.png/></alternatives></inline-formula>, an excited state <inline-formula><tex-math id=M9>begin{document}$6{rm{P}}_{3/2}$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M9.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M9.png/></alternatives></inline-formula>, and a Rydberg state <inline-formula><tex-math id=M10>begin{document}$n{rm{D}}_{5/2}$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M10.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M10.png/></alternatives></inline-formula> in a room-temperature cesium cell. A two-photon resonant Rydberg electromagnetic induced transparency (EIT) is used to optically detect the Rydberg level, in which a weak probe laser is locked at the resonant transition of <inline-formula><tex-math id=M11>begin{document}$|6{rm{S}}_{1/2}rangle rightarrow |6{rm{P}}_{3/2}rangle$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M11.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M11.png/></alternatives></inline-formula>, and a strong coupling laser drives the transition of <inline-formula><tex-math id=M12>begin{document}$|6{rm{P}}_{3/2}rangle rightarrow |n{rm{D}}_{5/2}rangle$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M12.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M12.png/></alternatives></inline-formula>. Both lasers are locked with a high-precision Fabry-Perot cavity. Two <i>E</i>-fields are incident into the vapor cell to interact with Rydberg atoms via a microwave horn, one is a strong microwave field with frequency 2.19 GHz, acting as a local field (<inline-formula><tex-math id=M13>begin{document}$E_{{rm{L}}}$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M13.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M13.png/></alternatives></inline-formula>) and resonantly coupling with two Rydberg energy levels, <inline-formula><tex-math id=M14>begin{document}$|68{rm{D}}_{5/2}rangle$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M14.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M14.png/></alternatives></inline-formula> and <inline-formula><tex-math id=M15>begin{document}$|69{rm{P}}_{3/2}rangle$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M15.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M15.png/></alternatives></inline-formula>, and the other is a weak signal field (<inline-formula><tex-math id=M16>begin{document}$E_{{rm{S}}}$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M16.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M16.png/></alternatives></inline-formula>) with frequency difference <inline-formula><tex-math id=M17>begin{document}${text{δ}} f$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M17.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M17.png/></alternatives></inline-formula>, interacting with the same Rydberg levels. The wave-absorbing material is placed around the vapor cell to reduce the reflection of microwave field. In the presence of the local field, the Rydberg atoms are employed as a microwave mixer for reading out the difference frequency <inline-formula><tex-math id=M18>begin{document}${text{δ}}f$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M18.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M18.png/></alternatives></inline-formula> oscillation signal, which is proportional to the amplitude of weak signal field. The minimum detectable field of <inline-formula><tex-math id=M19>begin{document}$E_{0} = 1.7$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M19.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M19.png/></alternatives></inline-formula> μV/cm is obtained when the lock-in output reaches the base noise. We also measure the frequency resolution of the Rydberg mixer by changing the <inline-formula><tex-math id=M20>begin{document}${text{δ}} f$end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M20.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M20.png/></alternatives></inline-formula> with fixed <inline-formula><tex-math id=M21>begin{document}$ f_{rm ref} $end{document}</tex-math><alternatives><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M21.jpg/><graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=6-20201401_M21.png/></alternatives></inline-formula>, thus achieving a frequency resolution better than 1 Hz. For neighboring fields with 1 Hz away from the signal field, an isolation of 60 dB is achieved. Furthermore, we use the Rydberg atom as an antenna to receive the baseband signals encoded into the weak microwave field, demonstrating that the receiver has a transmission bandwidth of about 200 MHz. The demonstration of sensitivity of Rydberg atoms to microwave field is particularly useful in many areas, such as quantum precise measurement and quantum communications. In general, this technique can be extended to the detection of electromagnetic radiation from the radio-frequency regime to the tera-hertz range and is feasible for fabricating a miniaturized devices, thereby providing us with a way to receive the information encoded in tera-hertz carriers in future work." @default.
• W3135453966 created "2021-03-15" @default.
• W3135453966 creator A5015603102 @default.
• W3135453966 creator A5030011300 @default.
• W3135453966 creator A5055923679 @default.
• W3135453966 creator A5072452652 @default.
• W3135453966 creator A5079422735 @default.
• W3135453966 creator A5085689718 @default.
• W3135453966 date "2021-01-01" @default.
• W3135453966 modified "2023-10-04" @default.
• W3135453966 title "High-sensitive microwave sensor and communication based on Rydberg atoms" @default.
• W3135453966 cites W2012424600 @default.
• W3135453966 cites W2014124991 @default.
• W3135453966 cites W2017198077 @default.
• W3135453966 cites W2020750445 @default.
• W3135453966 cites W2023318827 @default.
• W3135453966 cites W2051751652 @default.
• W3135453966 cites W2056329548 @default.
• W3135453966 cites W2080559570 @default.
• W3135453966 cites W2085231553 @default.
• W3135453966 cites W2104502349 @default.
• W3135453966 cites W2122053186 @default.
• W3135453966 cites W2122789651 @default.
• W3135453966 cites W2789367275 @default.
• W3135453966 cites W2794743895 @default.
• W3135453966 cites W2923281033 @default.
• W3135453966 cites W2944427797 @default.
• W3135453966 cites W2962784357 @default.
• W3135453966 cites W2963308816 @default.
• W3135453966 cites W2988294545 @default.
• W3135453966 cites W2999885395 @default.
• W3135453966 cites W3003381395 @default.
• W3135453966 cites W3004690261 @default.
• W3135453966 cites W3005532222 @default.
• W3135453966 cites W3009363176 @default.
• W3135453966 cites W3021749665 @default.
• W3135453966 cites W3022433452 @default.
• W3135453966 cites W3037952079 @default.
• W3135453966 cites W3099724639 @default.
• W3135453966 cites W3100806883 @default.
• W3135453966 cites W3102926457 @default.
• W3135453966 cites W3106020132 @default.
• W3135453966 cites W3106045281 @default.
• W3135453966 doi "https://doi.org/10.7498/aps.70.20201401" @default.
• W3135453966 hasPublicationYear "2021" @default.
• W3135453966 type Work @default.
• W3135453966 sameAs 3135453966 @default.
• W3135453966 citedByCount "4" @default.
• W3135453966 countsByYear W31354539662022 @default.
• W3135453966 countsByYear W31354539662023 @default.
• W3135453966 crossrefType "journal-article" @default.
• W3135453966 hasAuthorship W3135453966A5015603102 @default.
• W3135453966 hasAuthorship W3135453966A5030011300 @default.
• W3135453966 hasAuthorship W3135453966A5055923679 @default.
• W3135453966 hasAuthorship W3135453966A5072452652 @default.
• W3135453966 hasAuthorship W3135453966A5079422735 @default.
• W3135453966 hasAuthorship W3135453966A5085689718 @default.
• W3135453966 hasBestOaLocation W31354539661 @default.
• W3135453966 hasConcept C121332964 @default.
• W3135453966 hasConcept C145148216 @default.
• W3135453966 hasConcept C198291218 @default.
• W3135453966 hasConcept C33923547 @default.
• W3135453966 hasConcept C62520636 @default.
• W3135453966 hasConcept C70747811 @default.
• W3135453966 hasConceptScore W3135453966C121332964 @default.
• W3135453966 hasConceptScore W3135453966C145148216 @default.
• W3135453966 hasConceptScore W3135453966C198291218 @default.
• W3135453966 hasConceptScore W3135453966C33923547 @default.
• W3135453966 hasConceptScore W3135453966C62520636 @default.
• W3135453966 hasConceptScore W3135453966C70747811 @default.
• W3135453966 hasIssue "6" @default.
• W3135453966 hasLocation W31354539661 @default.
• W3135453966 hasOpenAccess W3135453966 @default.
• W3135453966 hasPrimaryLocation W31354539661 @default.
• W3135453966 hasRelatedWork W2000571018 @default.
• W3135453966 hasRelatedWork W2003062959 @default.
• W3135453966 hasRelatedWork W2079842361 @default.
• W3135453966 hasRelatedWork W2088361811 @default.
• W3135453966 hasRelatedWork W2092793634 @default.
• W3135453966 hasRelatedWork W2117232142 @default.
• W3135453966 hasRelatedWork W2512162291 @default.
• W3135453966 hasRelatedWork W2567397487 @default.
• W3135453966 hasRelatedWork W2752019705 @default.
• W3135453966 hasRelatedWork W3093386204 @default.
• W3135453966 hasVolume "70" @default.
• W3135453966 isParatext "false" @default.
• W3135453966 isRetracted "false" @default.
• W3135453966 magId "3135453966" @default.
• W3135453966 workType "article" @default.