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. Author manuscript; available in PMC: 2017 Dec 1.
Published in final edited form as: J Magn Reson. 2016 Sep 27;273:40–46. doi: 10.1016/j.jmr.2016.09.021

Fig. 4.

Fig. 4

1D GMO-TEDOR pulse sequence used for finding the offset and RF power response of GA-optimized phase modulation set. We studied the offset and RF power response for XX8, XY8, GA8x4 and GA10 phase modulations by using these phase values at φ1 to 4. The responses were measured by varying the offset and RF power of the recoupling π sequences on the 15N channel. A weak proton field of strength ωrf = ωr during the z-filters facilitates rapid dephasing of 13C spin coherences. The narrow and wide filled rectangles represent π=2 and π pulses respectively. The adopted phase cycles are: θ1 = 1111, θ2 = 2222, θ3 = θ6 = 1111, θ4 = θ7 = 1111, θ5 = 1111, θ8 = 2244, θ9 = 1111, θrec = 4224.