{"title":"Toward a Laser-Free Diamond Magnetometer for Microwave Fields","authors":"Pengju Zhao, Haodong Wang, Fei Kong, Zhecheng Wang, Yuhang Guo, Huiyao Yu, Fazhan Shi, Jiangfeng Du","doi":"10.1002/qute.202300191","DOIUrl":null,"url":null,"abstract":"<p>The nitrogen-vacancy (NV) center in diamond is a unique magnetometer. Its atomic size enables integrations of a tremendous amount (<span></span><math>\n <semantics>\n <msub>\n <mi>n</mi>\n <mi>NV</mi>\n </msub>\n <annotation>$n_{\\rm NV}$</annotation>\n </semantics></math>) of NV centers in a bulk diamond with a sensitivity scaling as <span></span><math>\n <semantics>\n <mrow>\n <mn>1</mn>\n <mo>/</mo>\n <msqrt>\n <msub>\n <mi>n</mi>\n <mi>NV</mi>\n </msub>\n </msqrt>\n </mrow>\n <annotation>$1/\\sqrt {n_{\\rm NV}}$</annotation>\n </semantics></math>. However, such a bulk sensor requires a high-power laser to polarize and read out the NV centers. The increasing thermal damage and additional noises associated with high-power lasers hinder the growth of <span></span><math>\n <semantics>\n <msub>\n <mi>n</mi>\n <mi>NV</mi>\n </msub>\n <annotation>$n_{\\rm NV}$</annotation>\n </semantics></math>, and thus limit the sensitivity at picotesla level. Here, it shows a relaxometry-based microwave magnetometer that the power density is determined by the relaxation time <span></span><math>\n <semantics>\n <msub>\n <mi>T</mi>\n <mn>1</mn>\n </msub>\n <annotation>$T_1$</annotation>\n </semantics></math>. By cooling the diamond sensor to prolong the <span></span><math>\n <semantics>\n <msub>\n <mi>T</mi>\n <mn>1</mn>\n </msub>\n <annotation>$T_1$</annotation>\n </semantics></math> (<span></span><math>\n <semantics>\n <mo>≈</mo>\n <annotation>$\\approx$</annotation>\n </semantics></math>s), the required power density further reduces to <span></span><math>\n <semantics>\n <mrow>\n <mn>0.077</mn>\n <mspace></mspace>\n <msup>\n <mi>Wcm</mi>\n <mrow>\n <mo>−</mo>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$0.077\\nobreakspace {\\rm Wcm^{-2}}$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <mrow>\n <mo>≈</mo>\n <mspace></mspace>\n <msup>\n <mn>10</mn>\n <mrow>\n <mo>−</mo>\n <mn>6</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$\\approx \\ 10^{-6}$</annotation>\n </semantics></math> of the saturation value. This work paves the way for the utilization of large-size diamond to promote the sensitivity of diamond magnetometer to femtotesla level and beyond.</p>","PeriodicalId":72073,"journal":{"name":"Advanced quantum technologies","volume":"8 4","pages":""},"PeriodicalIF":4.3000,"publicationDate":"2023-11-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced quantum technologies","FirstCategoryId":"1085","ListUrlMain":"https://advanced.onlinelibrary.wiley.com/doi/10.1002/qute.202300191","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"OPTICS","Score":null,"Total":0}
引用次数: 0
Abstract
The nitrogen-vacancy (NV) center in diamond is a unique magnetometer. Its atomic size enables integrations of a tremendous amount () of NV centers in a bulk diamond with a sensitivity scaling as . However, such a bulk sensor requires a high-power laser to polarize and read out the NV centers. The increasing thermal damage and additional noises associated with high-power lasers hinder the growth of , and thus limit the sensitivity at picotesla level. Here, it shows a relaxometry-based microwave magnetometer that the power density is determined by the relaxation time . By cooling the diamond sensor to prolong the (s), the required power density further reduces to , of the saturation value. This work paves the way for the utilization of large-size diamond to promote the sensitivity of diamond magnetometer to femtotesla level and beyond.