Cavity-enhanced room-temperature high sensitivity optical Faraday magnetometry
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文摘
We propose a cavity QED system with two-photon Doppler-free configuration for weak magnetic field detection with high sensitivity at room temperature based on cavity electromagnetically induced transparency. Owing to the destructive interference induced by the control and driving fields, two transparency channels are opened. The Faraday rotation within two transparency channels can be used to detect weak magnetic field with high sensitivity at room temperature. The sensitivity with single photon and multiphoton probe inputs is analyzed. With single photon measurement, our numerical calculations demonstrate that the sensitivity with class="mathmlsrc">class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0375960116309641&_mathId=si1.gif&_user=111111111&_pii=S0375960116309641&_rdoc=1&_issn=03759601&md5=933d129665371f10926050353e2465eb">class="imgLazyJSB inlineImage" height="16" width="73" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0375960116309641-si1.gif">class="mathContainer hidden">class="mathCode">3.8ace width="0.25em">ace>nT/Hz and class="mathmlsrc">class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0375960116309641&_mathId=si2.gif&_user=111111111&_pii=S0375960116309641&_rdoc=1&_issn=03759601&md5=7f749c55d73c7cbfc6464d25fbd8ffe9">class="imgLazyJSB inlineImage" height="16" width="72" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0375960116309641-si2.gif">class="mathContainer hidden">class="mathCode">6.4ace width="0.25em">ace>nT/Hz could be achieved. When we measure the magnetic field with multiphoton input, the sensitivity can be improved to class="mathmlsrc">class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0375960116309641&_mathId=si3.gif&_user=111111111&_pii=S0375960116309641&_rdoc=1&_issn=03759601&md5=ba52dceb67af22ddf1d090a4270e3fc5">class="imgLazyJSB inlineImage" height="16" width="70" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0375960116309641-si3.gif">class="mathContainer hidden">class="mathCode">7.7ace width="0.25em">ace>fT/Hz and class="mathmlsrc">class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0375960116309641&_mathId=si4.gif&_user=111111111&_pii=S0375960116309641&_rdoc=1&_issn=03759601&md5=0e6bbbaa628834104953462e0dc97b67">class="imgLazyJSB inlineImage" height="16" width="78" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0375960116309641-si4.gif">class="mathContainer hidden">class="mathCode">25.6ace width="0.25em">ace>fT/Hz under the realistic experimental conditions.

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