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arXiv:2610.39693

Optimized Dynamical Decoupling for Spin Ensembles with Large Inhomogeneities

Rajan Paul, Genko Genov, Oliver Schmid, Shinobu Onoda, Yutaka Kobayashi, Junichi Isoya, Fedor Jelezko

quant-phSubmitted Oct 29, 2026• Announced Oct 30, 2026• 0 citations
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Abstract

Spin ensembles show increasing promise for highly efficient quantum sensing and quantum technologies. However, protecting their coherent properties remains a significant challenge. Dynamical decoupling (DD) typically employs a sequence of fast pulses that aim to reduce the effect of unwanted system-environment interactions. However, the performance of the DD sequences typically suffers in spin ensembles, e.g., due to amplitude and frequency inhomogeneities and control errors. In this work, we compare the performance of an extensive number of DD protocols for coherence protection and quantum sensing in an ensemble of negatively charged NV centers under ambient conditions. We identify the optimal approach that uses rapid adiabatic passage pulses, which are robust to amplitude and frequency inhomogeneity, in combination with the variation of their phases. We experimentally demonstrate an improved signal contrast and an order-of-magnitude increase in memory time with the optimal sequence compared to the widely used XY8 with standard rectangular pulses. We also apply our approach for improved sensing of a weak oscillating field. While our particular demonstration is with NV centers in diamond, the optimized protocol is generally applicable to other spin ensembles and to systems with high amplitude and/or frequency inhomogeneities.

AI Summary

The paper asks how to preserve coherence and perform AC magnetometry in spin ensembles with large microwave-amplitude and resonance-frequency inhomogeneities. It experimentally compares dynamical-decoupling sequences in a room-temperature NV-diamond ensemble at a $1.1$ mT bias field, including XY8/XY16, composite-pulse protocols, interaction-decoupling sequences, smooth amplitude envelopes, and frequency-chirped rapid adiabatic passage (RAP) pulses. The measured relative drive-amplitude inhomogeneity is approximately $27\%$. The best-performing tested combination is KDD16 with Allen–Eberly RAP pulses and half-RAP preparation/readout. Numerical simulations and experimental parameter scans select a $1\,\mu\mathrm{s}$ pulse duration and $7.5$ MHz chirp range. At fixed pulse-center spacing of $1\,\mu\mathrm{s}$, exponential fits give coherence decay times of $49\,\mu\mathrm{s}$ for rectangular-pulse XY8, $131\,\mu\mathrm{s}$ for rectangular-pulse KDD16, $262\,\mu\mathrm{s}$ for sine-shaped KDD16, and $565\,\mu\mathrm{s}$ for KDD16-RAP. RAP-based population oscillations also increase readout contrast from about $17\%$ to $24.5\%$. Amplitude sensing is demonstrated with a non-phase-matched $500$ kHz test field: Bessel-modulated decay fits recover the expected field-amplitude scaling, and weaker applied signals are distinguishable than with rectangular XY8. Frequency scans identify the applied resonance but also show spurious responses that persist under pulse-phase randomization. Larger chirp ranges improve initial contrast while shortening coherence, attributed provisionally to leakage. The optimal sequence depends on the experimental errors; demonstrations are limited to this NV ensemble, and the sensing results do not establish an absolute magnetic sensitivity.

Little sign of AI-generated textIncrementalUnclear novelty

Error found: The claimed optimality is conditional on the tested apparatus and configurations, since the memory comparison uses an interpulse spacing optimized with XY8 rather than independently optimizing every protocol. Figure 2 inconsistently defines N as sequence repetitions while using t = Nτ, although the stated KDD16 construction contains 80 constituent pulses per repetition. Appendix Fig. A.9 incorrectly reports the Hahn-echo coherence time as 15.5 μs despite locating the exponential 1/e decay at a total evolution time of 31 μs. The Bloch-equation torque vector contains an erroneous factor of 1/2 and is inconsistent with its subsequently stated magnitude.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

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19 pages, 15 figures

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Spin ensembles show increasing promise for highly efficient quantum sensing and quantum technologies. However, protecting their coherent properties remains a significant challenge. Dynamical decoupling (DD) typically employs a sequence of fast pulses that aim to reduce the effect of unwanted system-environment interactions. However, the performance of the DD sequences typically suffers in spin ensembles, e.g., due to amplitude and frequency inhomogeneities and control errors. In this work, we compare the performance of an extensive number of DD protocols for coherence protection and quantum sensing in an ensemble of negatively charged NV centers under ambient conditions. We identify the optimal approach that uses rapid adiabatic passage pulses, which are robust to amplitude and frequency inhomogeneity, in combination with the variation of their phases. We experimentally demonstrate an improved signal contrast and an order-of-magnitude increase in memory time with the optimal sequence compared to the widely used XY8 with standard rectangular pulses. We also apply our approach for improved sensing of a weak oscillating field. While our particular demonstration is with NV centers in diamond, the optimized protocol is generally applicable to other spin ensembles and to systems with high amplitude and/or frequency inhomogeneities.
The paper asks how to preserve coherence and perform AC magnetometry in spin ensembles with large microwave-amplitude and resonance-frequency inhomogeneities. It experimentally compares dynamical-decoupling sequences in a room-temperature NV-diamond ensemble at a 1.11.11.1 mT bias field, including XY8/XY16, composite-pulse protocols, interaction-decoupling sequences, smooth amplitude envelopes, and frequency-chirped rapid adiabatic passage (RAP) pulses. The measured relative drive-amplitude inhomogeneity is approximately 27%27\%27%.
The best-performing tested combination is KDD16 with Allen–Eberly RAP pulses and half-RAP preparation/readout. Numerical simulations and experimental parameter scans select a 1 μs1\,\mu\mathrm{s}1μs pulse duration and 7.57.57.5 MHz chirp range. At fixed pulse-center spacing of 1 μs1\,\mu\mathrm{s}1μs, exponential fits give coherence decay times of 49 μs49\,\mu\mathrm{s}49μs for rectangular-pulse XY8, 131 μs131\,\mu\mathrm{s}131μs for rectangular-pulse KDD16, 262 μs262\,\mu\mathrm{s}262μs for sine-shaped KDD16, and 565 μs565\,\mu\mathrm{s}565μs for KDD16-RAP. RAP-based population oscillations also increase readout contrast from about 17%17\%17% to 24.5%24.5\%24.5%.
Amplitude sensing is demonstrated with a non-phase-matched 500500500 kHz test field: Bessel-modulated decay fits recover the expected field-amplitude scaling, and weaker applied signals are distinguishable than with rectangular XY8. Frequency scans identify the applied resonance but also show spurious responses that persist under pulse-phase randomization. Larger chirp ranges improve initial contrast while shortening coherence, attributed provisionally to leakage. The optimal sequence depends on the experimental errors; demonstrations are limited to this NV ensemble, and the sensing results do not establish an absolute magnetic sensitivity.
In this work, we optimize a dynamical decoupling (DD) protocol to improve the spin coherence properties of a dense ensemble of nitrogen-vacancy (NV) centers in diamond. Using liquid nitrogen-based cooling and DD microwave pulses, we increase the transverse coherence time T2 from ∼ 0.7 ms up to ∼ 30 ms. We extend previous work of single-axis (Carr-Purcell-Meiboom-Gill) DD towards the preservation of arbitrary spin states. After performing a detailed analysis of pulse and detuning errors, we compare the performance of various DD protocols. We identify that the concatenated XY8 pulse sequences serves as the optimal control scheme for preserving an arbitrary spin state. Finally, we use the concatenated sequences to demonstrate an immediate improvement of the AC magnetic sensitivity up to a factor of two at 250 kHz. For future work, similar protocols may be used to increase coherence times up to NV-NV interaction time scales, a major step toward the creation of quantum collective NV spin states.
We demonstrate significant improvements of the spin coherence time of a dense ensemble of nitrogen-vacancy (NV) centers in diamond through optimized dynamical decoupling (DD). Cooling the sample down to 77 K suppresses longitudinal spin relaxation T1{T}_{1}T1​ effects and DD microwave pulses are used to increase the transverse coherence time T2{T}_{2}T2​ from $\ensuremath{\sim}0.7\phantom{\rule{0.28em}{0ex}}\mathrm{ms}$ up to $\ensuremath{\sim}30\phantom{\rule{0.28em}{0ex}}\mathrm{ms}$. We extend previous work of single-axis (Carr-Purcell-Meiboom-Gill) DD towards the preservation of arbitrary spin states. Following a theoretical and experimental characterization of pulse and detuning errors, we compare the performance of various DD protocols. We identify that the optimal control scheme for preserving an arbitrary spin state is a recursive protocol, the concatenated version of the XY8 pulse sequence. The improved spin coherence might have an immediate impact on improvements of the sensitivities of ac magnetometry. Moreover, the protocol can be used on denser diamond samples to increase coherence times up to NV-NV interaction time scales, a major step towards the creation of quantum collective NV spin states.
Ensembles of nitrogen-vacancy (NV) centers in diamond are widely used as AC magnetometers. While such measurements are usually performed using standard (XY) dynamical decoupling (DD) protocols at room temperature, we study the sensitivities achieved by utilizing various DD protocols, for measuring magnetic AC fields at frequencies in the 10-250 kHz range, at room temperature and 77 K. By performing measurements on an isotopically pure 12^{12}12C sample, we find that the Carr-Purcell-Meiboom-Gill (CPMG) protocol, which is not robust against pulse imperfections, is less efficient for magnetometry than robust XY-based sequences. The concatenation of a standard XY-based protocol may enhance the sensitivities only for measuring high-frequency fields, for which many (>500> 500>500) DD pulses are necessary and the robustness against pulse imperfections is critical. Moreover, we show that cooling is effective only for measuring low-frequency fields (~10 kHz), for which the experiment time apporaches T1T_1T1​ at a small number of applied DD pulses.
The sensitivity of practical solid quantum sensing can be boosted up by increasing the number of probes. However, the effects of spin dephasing caused by inhomogeneous broadening and imperfect quantum control can reduce the fidelity of quantum control and the sensitivity of quantum sensing with the dense ensemble of probes, such as nitrogen-vacancy (NV) centers in diamond. Here, we present a robust and effective composite-pulse for high fidelity operation against inhomogeneous broadening and control errors via optimized modulation of the control field. Such a composite-pulse was verified on NV center to keep high fidelity quantum control up to a spectrum detuning as large as 110% of Rabi frequency. The sensitivity of the magnetometer with NV center ensemble was experimentally improved by a factor of 4, comparing to dynamical decoupling with a normal rectangular pulse. Our work marks an important step towards high trustworthy ultra-sensitive quantum sensing with imperfect quantum control in practical applications. The used principle is universal and not restricted to NV center ensemble magnetometer.
We perform a detailed theoretical-experimental study of the dynamical decoupling (DD) of the nitrogen-vacancy (NV) center in diamond. We investigate the DD sequences applied to suppress the dephasing of the electron spin of the NV center induced by the coupling to a spin bath composed of the substitutional nitrogen atoms. The decoupling efficiency of various DD schemes is studied, including both periodic and aperiodic pulse sequences. For ideal control pulses, we find that the DD protocols with the Carr-Purcell-Meiboom-Gill (CPMG) timing of the pulses provides best performance. We show that, as the number of control pulses increases, the decoupling fidelity scaling differs qualitatively from the predictions of the Magnus expansion, and explain the origin of this difference. In particular, more advanced symmetrized or concatenated protocols do not improve the DD performance. Next, we investigate the impact of the systematic instrumental pulse errors in different periodic and aperiodic pulse sequences. The DD protocols with the single-axis control do not preserve all spin components in the presence of the pulse errors, and the two-axis control is needed. We demonstrate that the two-axis control sequence with the CPMG timing is very robust with respect to the pulse errors. The impact of the pulse errors can be diminished further by symmetrizing this protocol. For all protocols studied here, we present a detailed account of the pulse error parameters which make the strongest impact on the DD performance. In conclusion, we give specific recommendations about choosing the decoupling protocol for the system under investigation.
Quantum sensing with solid-state spins has attracted considerable attention following the development of single quantum systems. In particular, sub-picotesla level magnetometry has been demonstrated using negatively-charged nitrogen-vacancy (NV) centers in diamond by increasing the number of spins simultaneously employed for sensing. However, scaling up the number of spins inevitably introduces inhomogeneities in detuning and control field amplitudes across the ensemble system, which degrades the achievable sensitivity. Although several techniques, including pulsed dynamical decoupling and shaped pulses, have been studied to overcome such noises, they are not generally compatible with GHz-range AC magnetometry based on Rabi oscillations. This dissertation presents the development of an experimental platform and the demonstration of robust GHz-range AC magnetometry using a large ensemble of NV centers under inhomogeneous fields. Particular emphasis is placed on the effects of control-field amplitude inhomogeneity. To improve the homogeneity of the control field, barrel-shaped microwave forming systems are experimentally characterized, and their performance is compared with that of planar systems. Then, to mitigate detuning noise as well as control-field amplitude noise, concatenated continuous dynamical decoupling (CCDD) is applied to the inhomogeneous ensemble system, and the resulting dynamics are investigated with several initial states prepared with composite pulses. Finally, the CCDD sequence is applied for GHz-range AC magnetometry and compared with the conventional direct Rabi method. The results demonstrate that the robust dressed states generated by CCDD extend the lower bound of measurable amplitudes in GHz-range AC magnetometry.