2002
DOI: 10.1103/physrevlett.89.130801
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High-Sensitivity Atomic Magnetometer Unaffected by Spin-Exchange Relaxation

Abstract: Alkali-metal magnetometers compete with SQUID detectors as the most sensitive magnetic field sensors. Their sensitivity is limited by relaxation due to spin-exchange collisions. We demonstrate a K magnetometer in which spin-exchange relaxation is completely eliminated by operating at high K density and low magnetic field. Direct measurements of the signal-to-noise ratio give a magnetometer sensitivity of 10 fT Hz(-1/2), limited by magnetic noise produced by Johnson currents in the magnetic shields. We extend a… Show more

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Cited by 869 publications
(651 citation statements)
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References 17 publications
(19 reference statements)
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“…For samples with a finite concentration of 13 C nuclear spin impurities, this technique revealed an orderof-magnitude suppression of the N electronic spin-bath dynamics, which can be explained by random interactions between proximal electronic and 13 C nuclear spin impurities. This spin-bath suppression enhances the efficacy of dynamical decoupling for samples with high N impurity concentration, enabling increased NV spin coherence times and thus realization of a FOM ~2×10 14 (ms cm − 3 ), which is within an order of magnitude of the state-of-the-art spin coherence FOM achieved in atomic systems 15 . Further optimization of the multi-spin-qubit FOM may be possible by engineering this spin-bath suppression, for example, with 13 C concentration higher than the natural value.…”
Section: Discussionmentioning
confidence: 80%
See 1 more Smart Citation
“…For samples with a finite concentration of 13 C nuclear spin impurities, this technique revealed an orderof-magnitude suppression of the N electronic spin-bath dynamics, which can be explained by random interactions between proximal electronic and 13 C nuclear spin impurities. This spin-bath suppression enhances the efficacy of dynamical decoupling for samples with high N impurity concentration, enabling increased NV spin coherence times and thus realization of a FOM ~2×10 14 (ms cm − 3 ), which is within an order of magnitude of the state-of-the-art spin coherence FOM achieved in atomic systems 15 . Further optimization of the multi-spin-qubit FOM may be possible by engineering this spin-bath suppression, for example, with 13 C concentration higher than the natural value.…”
Section: Discussionmentioning
confidence: 80%
“…In characterizing the potential usefulness of multi-qubit systems for quantum applications, the product of the qubit density (n qb ) and the qubit coherence lifetime (T 2 ) serves as a basic figure-of-merit (FOM), FOM = n qb T 2 . For example, in quantum measurements the phase-shift sensitivity δφ scales as 1/ FOM 5,[13][14][15] . Increasing this multi-qubit FOM requires an understanding of the sources of decoherence in the system and their interplay with qubit density.…”
mentioning
confidence: 99%
“…Several mechanisms of comparable importance have been identified for such relaxation [30], but some aspects of this process remain poorly understood [31]. The measured spin-destruction cross-sections are smaller for lighter alkali-metal atoms and result in a fundamental limit on the sensitivity of a K magnetometer of about 10 −17 V −1/2 T/Hz 1/2 [32], where V is the active volume of the sensor in cm 3 .…”
Section: General Features and Limits Of Sensitivity Of Optical Mamentioning
confidence: 99%
“…Nuclear magnetic resonance and magnetic resonance imaging are essential tools for both the physical and life sciences [1,2], but have been limited to the detection of large ensembles of spins due to their low sensitivity [3,4], or the macroscopic nature of sensors [5,6]. Over the past decades, significant efforts [7][8][9][10][11] have been directed toward pushing this sensitivity to its ultimate physical limit, the detection of individual nuclear spin signals localized in a small volume.…”
mentioning
confidence: 99%