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arXiv:2610.35016

From Single Spins to Ensembles: A Calibrated Symbolic Regression Pipeline for NV Spectroscopy

Evan Zhang, Zhenghang Zhi, Zewei Wang, Zeheng Wang

quant-phcs.AISubmitted Oct 26, 2026• Announced Oct 27, 2026• 0 citations
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Abstract

Characterizing nitrogen-vacancy (NV) ensembles requires connecting their collective spectra to individual centers that experience different local environments. We develop a symbolic-regression pipeline that carries single-center spin structure into a calibrated ensemble model by generating individual spectral responses and combining them with explicit weights. A constrained search selects Hermitian operator terms from single-center optically detected magnetic resonance spectra, fits their coefficients, and retains the selected expressions as source models for the ensemble. Ensemble calibration then accounts for resonance shifts, local disorder, orientation, and optical response while keeping the individual spectral contributions accessible. On public single-center and ensemble data, the zero-field ensemble held-frequency root-mean-square error decreases from 0.008835 to 0.003872 in normalized photoluminescence, a 56.2% improvement over matched uncorrected composition. In controlled QuTiP ensembles of 128 sites spanning four NV orientations, models calibrated at 0 and 3 mT predict an independently held-out 5.17 mT spectrum with errors of 0.000207-0.000228 across three random seeds, comparable to the 0.000200 noise standard deviation. Resolving the simulated response into its individual-center contributions shows how local spectral diversity combines into the ensemble line shape. By retaining the source Hamiltonians while calibrating sample-dependent spectral differences, the pipeline connects local spin physics to collective optical readout and makes the contributions to an ensemble line shape available for physical interpretation.

AI Summary

The paper addresses how to connect individual nitrogen-vacancy (NV) center spin models to ensemble optically detected magnetic resonance spectra when centers have different local environments. It proposes a symbolic-regression pipeline that selects Hermitian operator terms from single-center spectra, fits their coefficients, and retains the resulting Hamiltonians as source models. Individual spectral responses are combined with explicit weights, followed by ensemble calibration for resonance shifts, local disorder, orientation, and optical response. The construction keeps individual-center spectral contributions accessible rather than representing only the aggregate line shape. Validation uses public single-center and ensemble data, together with controlled QuTiP simulations. For a zero-field experimental ensemble spectrum, the root-mean-square error on held-out frequencies decreases from $0.008835$ to $0.003872$ in normalized photoluminescence, a reported $56.2\%$ reduction relative to matched uncorrected composition. In simulated ensembles containing $128$ sites across four NV orientations, calibration at $0$ and $3\,\mathrm{mT}$ yields prediction errors of $0.000207$–$0.000228$ at an independently held-out field of $5.17\,\mathrm{mT}$ across three random seeds, compared with a noise standard deviation of $0.000200$. The simulated response is also decomposed into individual-center contributions to examine how local spectral diversity produces the ensemble line shape. The abstract does not state explicit limitations. Its reported held-out-field validation is simulation-based; the reported experimental test concerns held-out frequencies at zero field. Further methodological details and limitations cannot be assessed from the abstract alone.

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Characterizing nitrogen-vacancy (NV) ensembles requires connecting their collective spectra to individual centers that experience different local environments. We develop a symbolic-regression pipeline that carries single-center spin structure into a calibrated ensemble model by generating individual spectral responses and combining them with explicit weights. A constrained search selects Hermitian operator terms from single-center optically detected magnetic resonance spectra, fits their coefficients, and retains the selected expressions as source models for the ensemble. Ensemble calibration then accounts for resonance shifts, local disorder, orientation, and optical response while keeping the individual spectral contributions accessible. On public single-center and ensemble data, the zero-field ensemble held-frequency root-mean-square error decreases from 0.008835 to 0.003872 in normalized photoluminescence, a 56.2% improvement over matched uncorrected composition. In controlled QuTiP ensembles of 128 sites spanning four NV orientations, models calibrated at 0 and 3 mT predict an independently held-out 5.17 mT spectrum with errors of 0.000207-0.000228 across three random seeds, comparable to the 0.000200 noise standard deviation. Resolving the simulated response into its individual-center contributions shows how local spectral diversity combines into the ensemble line shape. By retaining the source Hamiltonians while calibrating sample-dependent spectral differences, the pipeline connects local spin physics to collective optical readout and makes the contributions to an ensemble line shape available for physical interpretation.
The paper addresses how to connect individual nitrogen-vacancy (NV) center spin models to ensemble optically detected magnetic resonance spectra when centers have different local environments. It proposes a symbolic-regression pipeline that selects Hermitian operator terms from single-center spectra, fits their coefficients, and retains the resulting Hamiltonians as source models. Individual spectral responses are combined with explicit weights, followed by ensemble calibration for resonance shifts, local disorder, orientation, and optical response. The construction keeps individual-center spectral contributions accessible rather than representing only the aggregate line shape.
Validation uses public single-center and ensemble data, together with controlled QuTiP simulations. For a zero-field experimental ensemble spectrum, the root-mean-square error on held-out frequencies decreases from 0.0088350.0088350.008835 to 0.0038720.0038720.003872 in normalized photoluminescence, a reported 56.2%56.2\%56.2% reduction relative to matched uncorrected composition. In simulated ensembles containing 128128128 sites across four NV orientations, calibration at 000 and 3 mT3\,\mathrm{mT}3mT yields prediction errors of 0.0002070.0002070.000207–0.0002280.0002280.000228 at an independently held-out field of 5.17 mT5.17\,\mathrm{mT}5.17mT across three random seeds, compared with a noise standard deviation of 0.0002000.0002000.000200. The simulated response is also decomposed into individual-center contributions to examine how local spectral diversity produces the ensemble line shape.
The abstract does not state explicit limitations. Its reported held-out-field validation is simulation-based; the reported experimental test concerns held-out frequencies at zero field. Further methodological details and limitations cannot be assessed from the abstract alone.
Fiber-coupled ensembles of nanodiamonds containing nitrogen-vacancy (NV) centers are widely used for microscopic magnetic field measurements. However, the random distribution of NV crystal axes in nanodiamond ensembles causes resonance frequencies from differently oriented NV centers to overlap in the ODMR spectrum, distorting the spectral line shape and breaking the linear mapping between frequency shift and magnetic field. As a result, conventional magnetic field measurements based on Lorentzian fitting suffer from significant systematic errors. Here, we establish a fiber-nanodiamond ensemble model to analyze the impact of random NV orientations on the ODMR linear response and define an effective ensemble-averaged linear response coefficient K . Fisher information analysis identifies an information-optimal intrinsic magnetic field of approximately 640 µT, at which the ensemble response can be reliably approximated as linear in its vicinity. Building on this condition, we propose a model-assisted regression scheme, in which the physical fiber-nanodiamond ensemble model defines the optimal operating condition and the associated linear frequency-field scaling, while intrinsic-field-guided Gaussian regression (IFGGR) extracts magnetic-field-induced frequency shifts from distorted ensemble ODMR spectra, enabling accurate magnetic field estimation via the response coefficient K . Under identical acquisition conditions, the proposed method reduces the RMSE from 37.21 µT to 8.99 µT and significantly suppresses systematic bias, while achieving an absolute sensitivity approaching the shot-noise limit at optimal averaging time. The relative slope error reduction (≈15.6-fold) further confirms improved local linearity near the optimal operating point.
Nitrogen-vacancy (NV) center ensembles provide a powerful platform for high-precision temperature sensing, with ongoing efforts to further enhance their measurement performance. In ensemble NV optically detected magnetic resonance (ODMR) spectra, commonly used Lorentzian and Voigt fitting models fail to accurately describe the spectral shape near the resonance frequency, leading to degraded precision in resonance-frequency determination and, consequently, temperature estimation. In this work, we analytically establish a new fitting method, termed dip-peak fitting, for extracting the resonance frequency from ensemble cw-ODMR spectra. Starting from a physical model that describes ensemble cw-ODMR spectra as a convolution of single-NV responses with distributed zero-field splitting and strain, we show that the spectral feature near resonance can be accurately approximated by a single Lorentzian function with a background term. The proposed fitting model reproduces the cw-ODMR spectrum around resonance more faithfully than conventional approaches, enabling faster and more accurate resonance-frequency determination under weaker microwave excitation. Experiments using fluorescent nanodiamond ensembles confirm the robustness and applicability of this method for high-precision temperature sensing.
Nitrogen-vacancy (NV) centers in diamond exist in neutral (NV0) and negatively charged (NV-) states, and quantifying their respective photoluminescence (PL) contributions is important for charge-state-based measurements. Existing methods either require additional experimental control or may suffer from limited physical identifiability. Here, we introduce a geometric method for determining NV charge-state contributions from PL spectra acquired at different excitation intensities. Each spectrum is mapped into a low-dimensional space through broadband spectral weighting, where changes in the relative NV0 and NV- contributions trace a one-dimensional trajectory. Zero-phonon-line (ZPL) information from two spectra physically calibrates this trajectory, enabling the NV-PL contribution to be determined by geometric projection. Measurements on two bulk single-crystal diamond samples yielded NV- contributions in close agreement with those obtained using an independent dual-excitation reference-spectrum method, with root-mean-square errors of 1.11 and 0.31 percentage points. Under additive spectral noise, the proposed method exhibited more than an order of magnitude less variation than a ZPL-only method. Fisher-information analysis further showed that the three-dimensional CIE XYZ representation retained approximately 81% of the information about the NV- contribution available in the full spectrum. These results establish a physically calibrated approach to low-dimensional spectral estimation that combines reduced experimental overhead with robust parameter estimation and provides a general framework for spectral sensing governed by a small number of physical degrees of freedom.
Abstract Transverse-magnetic-field-induced spin mixing in nitrogen-vacancy (NV) centers hybridizes the |0⟩ and | ± 1⟩ manifolds, degrading optical spin polarization and spin-dependent fluorescence and thereby limiting optically detected magnetic resonance (ODMR) contrast and quantum-sensor fidelity. While recent work has clarified key elements of NV photophysics, how spin mixing evolves with temperature under device-relevant operating conditions─and how it intertwines with charge-state dynamics─remains insufficiently quantified. Here we perform systematic magnetic-field-temperature (B-T) mapping of transverse-field-induced photoluminescence (PL) quenching in an ensemble of NV centers. By spectrally resolving the NV– and NV0 zero-phonon-line emission, we disentangle spin-mixing-driven contrast loss within NV– from correlated changes in charge-state-resolved fluorescence. We introduce an operational critical field Bc extracted from the PL-contrast line shape, which provides a compact, reproducible figure-of-merit for transverse-field robustness and enables straightforward comparison across temperatures and field geometries. The measured temperature dependence of Bc is captured by a concise model incorporating phonon-mediated excited-state orbital dynamics, establishing a predictive framework for optimizing operating conditions and benchmarking ensemble NV sensing platforms.
Precise characterization of the local spin environment of single diamond nitrogen-vacancy (NV) centers is crucial for advancing quantum sensing, quantum networking, and the optimization of quantum materials. However, single NV center fluorescence measurements requires long averaging times to obtain clean data that is suitable for conventional model fitting, and that constitutes a key experimental bottleneck for high-throughput characterization. To address this, we introduce \textsc{NVRNet}, a physics-informed simulation-to-reality machine learning pipeline that maps minimal-sweep, noisy Ramsey data to a denoised waveform while directly estimating the hyperfine coupling to proximal 13C{}^{13}\mathrm{C}13C nuclear spins. The pipeline's denoiser utilizes a two-stage time-frequency U-Net and an attention-augmented time-domain U-Net, pretrained on Hamiltonian-based spin-dynamics simulations with experimentally calibrated noise. To effectively bridge the simulation-to-reality gap, parameter-efficient adapters are attached to the backbone and fine-tuned on targeted experimental data. Across three distinct NV centers, this experimentally fine-tuned model reduces the median reconstruction error on held-out, few-sweep traces to 0.44-0.67×0.44\text{-}0.67\times0.44-0.67× of the raw experimental noise level. Subsequently, a transformer-based estimator extracts the underlying hyperfine parameters. Forward reconstructions derived from these inferred parameters faithfully reproduce the dominant experimental time- and frequency-domain features, yielding representative normalized fast Fourier transform (FFT) reconstruction errors of 0.10-0.190.10\text{-}0.190.10-0.19. By reducing both the required data volume and acquisition time, \textsc{NVRNet} enables up to ∼40×\sim 40\times∼40× acceleration of the measurement process, establishing a fast, hardware-compatible pathway for robust hyperfine inference and autonomous qubit characterization.
The nitrogen-vacancy (NV) center in diamond is a solid-state spin defect that has been widely adopted for quantum sensing and quantum information processing applications. Typically, experiments are performed either with a single isolated NV center or with an unresolved ensemble of many NV centers, resulting in a trade-off between measurement speed and spatial resolution or control over individual defects. In this work, we introduce an experimental platform that bypasses this trade-off by addressing multiple optically resolved NV centers in parallel. We perform charge- and spin-state manipulations selectively on multiple NV centers from within a larger set, and we manipulate and measure the electronic spin states of over 100 NV centers in parallel. We show that the high signal-to-noise ratio of the measurements enables the detection of shot-to-shot pairwise correlations between the spin states of 108 NV centers, corresponding to the simultaneous measurement of 5778 unique correlation coefficients. We discuss how our platform can be scaled to parallel experiments with thousands of individually resolved NV centers. These results enable parallelized high-throughput sensing experiments that retain the spatial resolution of single defects and will, thereby, help to unlock advances in applications such as single-molecule NMR and characterization of integrated circuits. In addition, our approach to multiplexing provides a natural platform for the application of recently developed correlated sensing techniques.