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International Journal of Advanced Natural Sciences and Engineering Researches

Feedback Control over Response in the Cavity Quantum Electromagnetic Sensor

Sergey Borisenok

Published Jun 27, 2024• 0 citations
OpenAlex

Abstract

Here we discuss as an important particular case the hybrid quantum electromagnetic sensor represented by a nitrogen-vacancy (NV) ensemble of N gt;gt; 1 centers in the doped diamond coupled to a high-quality factor dielectric resonator. The existing NV ensemble-based devices exhibit sensitivities that are several orders of magnitude away from theoretical limits. On the one hand, improvements in spin dephasing time, readout accuracy, and properties of the base diamond material can significantly improve the quality of operation of a quantum sensor. On the other hand, sensing optimization schemes also significantly affect its performance. We focus on the application of feedback to control the response in the cavity quantum electromagnetic sensor. We use the standard Tavis-Cummings model for the system and then introduce control over the target attractor method. In this model they are considered to be noninteracting two-level systems with transition frequencies wj, distributed inhomogeneously due to heterogeneous local magnetic and strain environments as well as hyperfine coupling with 14N nuclear spins. We adopted an operator form of closed-loop algorithm to the semi-classical Tavis-Cummings model in its ‘weak microwave drive’ limit. We used here target attractor Kolesnikov’s formulation of feedback to track the sensor response r or, alternatively, the reflected signal to the input drive field. In both cases, we achieve the tracking goal in the exponentially fast convergence.

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International Journal of Advanced Natural Sciences and Engineering Researches•Jan 1, 2023•1 citation
Here we discuss as an important particular case the hybrid quantum electromagnetic sensor represented by a nitrogen-vacancy (NV) ensemble of N gt;gt; 1 centers in the doped diamond coupled to a high-quality factor dielectric resonator. The existing NV ensemble-based devices exhibit sensitivities that are several orders of magnitude away from theoretical limits. On the one hand, improvements in spin dephasing time, readout accuracy, and properties of the base diamond material can significantly improve the quality of operation of a quantum sensor. On the other hand, sensing optimization schemes also significantly affect its performance. We focus on the application of feedback to control the response in the cavity quantum electromagnetic sensor. We use the standard Tavis-Cummings model for the system and then introduce control over the target attractor method. In this model they are considered to be noninteracting two-level systems with transition frequencies wj, distributed inhomogeneously due to heterogeneous local magnetic and strain environments as well as hyperfine coupling with 14N nuclear spins. We adopted an operator form of closed-loop algorithm to the semi-classical Tavis-Cummings model in its ‘weak microwave drive’ limit. We used here target attractor Kolesnikov’s formulation of feedback to track the sensor response r or, alternatively, the reflected signal to the input drive field. In both cases, we achieve the tracking goal in the exponentially fast convergence.
Ultrasensitive quantum detection of external weak signals at the nanoscale levels can be implemented in a variety of forms. Here we discuss different feedback control algorithms for the sensing scenario based on the semiclassical Tavis-Cummings model for nitrogen-vacancy (NV) centers located in the diamond. In the frame of this model, the sensing elements are considered as non-interacting two-level quantum systems, distribute in-homogeneously due to heterogeneous local magnetic and strain environments. The dynamical system of ordinary differential equations corresponding to the model contains the set of control parameters: the detunings between the drive frequency and the cavity frequency and between the drive frequency and NV transition frequency, as well as the relaxation coefficients. Correspondingly, it opens a gate for developing feedback control algorithms for tracking the cavity field, the income signal, and the reflection signal in the model sensing system. To study the principal features of algorithmic feedback we formulate the simplified ’toy model’ for the Tavis-Cummings system and investigate alternative schemes of feedback (gradient methods, target attractor methods) to compare their pros and cons for effective control for nitrogen-vacancy-cavity quantum sensing based on different choices of the control parameter set. This work was supported by the Research Fund of Abdullah Gül University; Project Number: BAP FBA-2023-176 ’Geribesleme kontrol algoritmaları ile kubit tabanlı sensörlerin verimliliğinin artırılması’. The paper was presented at PhysCon2024.
The nitrogen-vacancy (NV) center in diamond is a quantum defect in diamond with unique properties for use in high-sensitive, high-resolution quantum sensors of magnetic fields. One of the most interesting and challenging application of NV quantum sensors is nanoscale magnetic resonance imaging (nano-MRI), which would enable to address single biomolecules. To this goal, improving the sensitivity of the NV sensor is a crucial task. Here, we present a quantum optimal control method that optimizes the sensitivity of NV sensor to specific weak magnetic signals with biologically-relevant, complex spectrum. The method, based on the mapping of the sensing problem on a problem of energy optimization of an Ising chain, allows us to improve sensitivity by three orders of magnitude compared to standard control sequences.
Solid-state quantum sensors based on ensembles of nitrogen-vacancy (NV) centers in diamond have emerged as powerful platforms for high-precision metrology. Coupling the NV ensemble to a microwave cavity mode in a cavity quantum electrodynamics (cQED) configuration enables spin readout that surpasses the limitations of conventional optical detection, achieving sub-picotesla magnetic sensitivities. However, existing continuous-wave cQED approaches remain far from the intrinsic spin-projection-noise limit due to spin saturation and power broadening. Here, we introduce a dispersive cQED readout technique to overcome these fundamental limitations in NV ensemble sensing. We develop a comprehensive theoretical framework describing the dispersive interaction and analyze the time-domain dynamics of a strongly-coupled NV-cavity system. Our results indicate near-unity inverse readout fidelity and femtotesla-level sensitivity using a commercially available diamond NV ensemble. Importantly, the dispersive readout exhibits a distinct sensitivity scaling that improves as 1/N with increasing number of spins N, providing a practical pathway toward approaching the standard quantum limit for solid-state spin-ensemble sensors.
Quantum magnetic sensors based on nitrogen-vacancy (NV) centers in diamond are expected to be applicable to biological and chemical applications However, their DC magnetic field sensitivity is still insufficient for demanding applications such as magnetoencephalography requiring extraordinary sensitivity. The spin dephasing time 𝑇2∗ is a key parameter to improve the sensitivity, but 𝑇2∗ of typical millimeter-scale NV centers is limited by magnetic field inhomogeneity, strain field inhomogeneity, and electronic spin bath. In this work, we developed (i) a magnet system suppressing both the longitudinal magnetic field and transverse strain field inhomogeneities and (ii) a microwave (MW) and radio-frequency (RF) application system for high-efficiency spin-bath driving (SBD) suitable for a diamond (111) sample.
The nitrogen-vacancy centers in diamond have exhibited excellent sensing capabilities. By applying the resonance frequency tracking (RFT) method in a closed-loop system, magnetic-field measurements with a wide dynamic range have been demonstrated. However, the previous strategies employ phase-sensitive control signals, which degrade control robustness and reduce tracking rates, thereby impeding real-time measurements. Here, an amplitude–phase joint discrimination strategy is proposed to improve robustness, overcoming the limitations of existing strategies that are sensitive to phase delays in fluorescence signal transmission. Moreover, to improve the tracking speed, a customized device, integrating a fast-response lock-in amplifier (LIA) and a frequency-agile microwave (MW) source, is reported. The LIA achieves a response time as short as 20 μs, while the MW source reaches a frequency switching time of 1 μs. The proposed strategy and customized device are implemented and evaluated on an all-fiber quantum current sensing system. Test results show that the system achieves a maximum sampling rate of 20 kHz, with excellent linearity (a linear deviation of 0.37% over the range of 0-120 A) and high accuracy (a measurement error of 0.73% at 80 A), making it promising for a wide range of high-speed quantum measurement scenarios.
Recent great progress in studying theoretical and especially experimental properties of BoseEinstein condensate (BEC) creates a new era in developing and designing principally novel types of quantum devices, including quantum sensors for measuring nonlinear interactions, external electrical and magnetic fields, and other physical characteristics with high sensitivity. Here we discuss the application of feedback control over a quantum sensor based on the Bose-Einstein condensate trapped in twodimensional ring potential. For a weakly interacting regime, the dynamics of such a system are modeled by three coupled complex differential master equations containing the parameter of interaction and the chemical potential parameter. The last one plays the role of control variable in sensing protocol for twobody interaction. The goal of control is to minimize the effects of the higher energy levels in BEC by driving their corresponding matrix density elements. The control algorithm is designed as Kolesnikov’s feedback forming an artificial target attractor in the dynamical system. We re-formulate Kolesnikov’s approach in the operator form to adapt it to quantum engineering processes. The control approach proposed here can be efficiently extended to different sensing protocols for detecting external magnetic fields, rotational components, and other physical characteristics of BEC interacting with the environment.