2014
DOI: 10.1103/physrevb.89.024404
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Long-lived selective spin echoes in dipolar solids under periodic and aperiodicπ-pulse trains

Abstract: The application of Carr-Purcell-Meiboom-Gill (CPMG) π−trains for dynamically decoupling a system from its environment has been extensively studied in a variety of physical systems. When applied to dipolar solids, recent experiments have demonstrated that CPMG pulse trains can generate long-lived spin echoes. While there still remains some controversy as to the origins of these long-lived spin echoes under the CPMG sequence, there is a general agreement that pulse errors during the π−pulses are a necessary requ… Show more

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Cited by 6 publications
(1 citation statement)
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“…3a–f), whereas under CP-Y (blue circles), the echo amplitude is rapidly reduced, owing to the limited available rf power resulting in deviation from the ideal hard pulses (see Supplementary Note 3). The contrasting behaviour of T 2 under alternating phase CP-X/Y has been observed in other systems 4446,48 and has been attributed variably to spin locking 48,49 or stimulated echoes 50 . Here, we ascribe the increase of T 2 under CP-X to a form of pulsed spin locking arising from dipolar evolution during the finite-duration π -pulses 49 : our interpretation is based on the observation that the spin lock disappears for small pulse-to-cycle time ratios t π / t c (see Supplementary Note 2).…”
Section: Resultsmentioning
confidence: 83%
“…3a–f), whereas under CP-Y (blue circles), the echo amplitude is rapidly reduced, owing to the limited available rf power resulting in deviation from the ideal hard pulses (see Supplementary Note 3). The contrasting behaviour of T 2 under alternating phase CP-X/Y has been observed in other systems 4446,48 and has been attributed variably to spin locking 48,49 or stimulated echoes 50 . Here, we ascribe the increase of T 2 under CP-X to a form of pulsed spin locking arising from dipolar evolution during the finite-duration π -pulses 49 : our interpretation is based on the observation that the spin lock disappears for small pulse-to-cycle time ratios t π / t c (see Supplementary Note 2).…”
Section: Resultsmentioning
confidence: 83%