Low‐load rotor‐synchronised Hahn‐echo pulse train (RS‐HEPT) 1H decoupling in solid‐state NMR: factors affecting MAS spin‐echo dephasing times
Low‐load rotor‐synchronised Hahn‐echo pulse train (RS‐HEPT) 1H decoupling in solid‐state NMR: factors affecting MAS spin‐echo dephasing times
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固态核磁共振中的低负载转子同步哈恩回波脉冲串(RS-HEPT)1H解耦:影响MAS自旋回波相移时间的因素
DOI:
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发表时间:
2007
期刊:
影响因子:
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通讯作者:
S. Brown
中科院分区:
文献类型:
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作者:
J. Griffin;C. Tripon;A. Samoson;C. Filip;S. Brown
Transverse dephasing times T2′ in spin‐echo MAS NMR using rotor‐synchronised Hahn‐echo pulse‐train (RS‐HEPT) low‐load 1H decoupling are evaluated. Experiments were performed at 300 and 600 MHz for 13CH‐labelled L‐alanine and 15NH(δ)‐labelled L‐histidine·HCl·H2O, together with SPINEVOLUTION simulations for a ten‐spin system representing the crystal structure environment of the 13CH carbon in L‐alanine. For 30 kHz MAS and ν1(1H) = 100 kHz at 300 MHz, a RS‐HEPT T2′ value of 17 ± 1 ms was obtained for 13CH‐labelled L‐alanine which is ∼50% of the XiX T2′ value of 33 ± 2 ms. Optimum RS‐HEPT decoupling performance is observed for a relative phase of alternate RS‐HEPT π–pulses, Δϕ = ϕ′− ϕ, between 40 and 60° . For experiments at 600 MHz and 30 kHz MAS with 13CH‐labelled L‐alanine, the best RS‐HEPT (ν1(1H) = 100 kHz) T2′ value was 3 times longer than that observed for low‐power continuously applied sequences with ν1(1H) ⩽40 kHz, i.e. corresponding to the same average power dissipated in the probe. A marked improvement in RS‐HEPT 1H decoupling is observed for increasing MAS frequency: at 55.6 kHz MAS, a best RS‐HEPT T2′ value of 34 ± 5 ms was recorded for 13CH‐labelled L‐alanine. Much improved RS‐HEPT broadband performance was also observed at 55.6 kHz MAS as compared to 30 kHz MAS. Copyright © 2007 John Wiley & Sons, Ltd.