David Cristea , Utsab Banerjee , Xiaoxun Chen , Julia C. Draeger , Dominik B. Bucher , Aharon Blank
{"title":"Dual-frequency dielectric resonator for combined magnetic resonance of g∼2 paramagnetic species and diamond NV centers","authors":"David Cristea , Utsab Banerjee , Xiaoxun Chen , Julia C. Draeger , Dominik B. Bucher , Aharon Blank","doi":"10.1016/j.jmro.2026.100220","DOIUrl":null,"url":null,"abstract":"<div><div>Nitrogen-vacancy (NV) centers in diamond are leading platforms for quantum sensing, yet efficient control of macroscopic ensembles remains challenging. While resonant structures offer high microwave-to-magnetic-field conversion factor (<em>C</em><sub>p</sub>), their narrow bandwidths typically preclude simultaneous addressing of NV transitions and co-located g∼2 paramagnetic species, which are separated by ∼2.87 GHz at X-band. By enabling concurrent pulsed control of NVs and bath electron spins, one can facilitate advanced applications such as spin-bath driving and NV-assisted dynamic nuclear polarization in ensemble samples. We present a compact dual-frequency dielectric resonator designed to resolve this limitation by co-exciting the TE<sub>01δ</sub> mode (∼9 GHz) and the HEM<sub>12δ</sub> mode (∼11.8 GHz) within a high-permittivity (<em>ε</em>' ∼ 80) ceramic ring. This architecture concentrates magnetic fields in a shared sample volume just above the resonator surface while maintaining essential optical access and minimizing electric-field-induced heating. Experimental characterization demonstrates resonance frequencies of 8.78 GHz (<em>Q ∼</em> 237) and 11.41 GHz (<em>Q</em> ∼ 64), with fine-tuning capabilities. Electron spin resonance (ESR) measurements on P1-rich diamond yielded microwave magnetic field, <em>B</em><sub>1</sub>, conversion factors of <em>C</em><sub>p</sub> ∼3.6 and ∼1.2 G/√W, for the respective modes. Additional validation via optically detected magnetic resonance (ODMR) confirmed high-fidelity Rabi oscillations for the low frequency mode (the NV transition |0>↔|-1>) π-pulse durations of ∼ 24 ns, using a peak microwave power of 63 W.</div></div>","PeriodicalId":365,"journal":{"name":"Journal of Magnetic Resonance Open","volume":"27 ","pages":"Article 100220"},"PeriodicalIF":2.2000,"publicationDate":"2026-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Magnetic Resonance Open","FirstCategoryId":"1","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2666441026000063","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2026/5/9 0:00:00","PubModel":"Epub","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Nitrogen-vacancy (NV) centers in diamond are leading platforms for quantum sensing, yet efficient control of macroscopic ensembles remains challenging. While resonant structures offer high microwave-to-magnetic-field conversion factor (Cp), their narrow bandwidths typically preclude simultaneous addressing of NV transitions and co-located g∼2 paramagnetic species, which are separated by ∼2.87 GHz at X-band. By enabling concurrent pulsed control of NVs and bath electron spins, one can facilitate advanced applications such as spin-bath driving and NV-assisted dynamic nuclear polarization in ensemble samples. We present a compact dual-frequency dielectric resonator designed to resolve this limitation by co-exciting the TE01δ mode (∼9 GHz) and the HEM12δ mode (∼11.8 GHz) within a high-permittivity (ε' ∼ 80) ceramic ring. This architecture concentrates magnetic fields in a shared sample volume just above the resonator surface while maintaining essential optical access and minimizing electric-field-induced heating. Experimental characterization demonstrates resonance frequencies of 8.78 GHz (Q ∼ 237) and 11.41 GHz (Q ∼ 64), with fine-tuning capabilities. Electron spin resonance (ESR) measurements on P1-rich diamond yielded microwave magnetic field, B1, conversion factors of Cp ∼3.6 and ∼1.2 G/√W, for the respective modes. Additional validation via optically detected magnetic resonance (ODMR) confirmed high-fidelity Rabi oscillations for the low frequency mode (the NV transition |0>↔|-1>) π-pulse durations of ∼ 24 ns, using a peak microwave power of 63 W.