Dual-frequency dielectric resonator for combined magnetic resonance of g∼2 paramagnetic species and diamond NV centers

IF 2.2
Journal of Magnetic Resonance Open Pub Date : 2026-06-01 Epub Date: 2026-05-09 DOI:10.1016/j.jmro.2026.100220
David Cristea , Utsab Banerjee , Xiaoxun Chen , Julia C. Draeger , Dominik B. Bucher , Aharon Blank
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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.
用于g ~ 2顺磁性物质和金刚石NV中心组合磁共振的双频介电谐振器
金刚石中的氮空位(NV)中心是量子传感的主要平台,但有效控制宏观系综仍然是一个挑战。虽然谐振结构提供高微波-磁场转换因子(Cp),但它们的窄带宽通常阻止同时寻址NV跃迁和共定位的g ~ 2顺磁物质,它们在x波段相隔约2.87 GHz。通过实现nv和电子自旋的同步脉冲控制,可以促进自旋-浴驱动和nv辅助的系综样品动态核极化等高级应用。我们提出了一种紧凑的双频介质谐振器,旨在通过在高介电常数(ε’~ 80)陶瓷环内共激励TE01δ模式(~ 9 GHz)和HEM12δ模式(~ 11.8 GHz)来解决这一限制。这种结构将磁场集中在谐振器表面上方的共享样本量中,同时保持基本的光学通道并最大限度地减少电场引起的加热。实验表征表明共振频率为8.78 GHz (Q ~ 237)和11.41 GHz (Q ~ 64),具有微调能力。在富含p1的金刚石上进行电子自旋共振(ESR)测量,得到微波磁场B1,转换因子分别为Cp ~ 3.6和~ 1.2 G/√W。通过光学探测磁共振(ODMR)的进一步验证证实了低频模式(NV跃迁|-1>;)的高保真拉比振荡,其π脉冲持续时间为~ 24 ns,峰值微波功率为63 W。
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来源期刊
CiteScore
1.90
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0.00%
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