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. Author manuscript; available in PMC: 2013 Sep 3.
Published in final edited form as: J Magn Reson. 2012 Apr 26;220:54–61. doi: 10.1016/j.jmr.2012.04.008

Fig. 9.

Fig. 9

Two-dimensional PDLF pulse sequences. The pulse sequences in Fig. 1B are modified to perform PDLF class experiments by the addition of a π pulse on the 1H channel at the same position as the 15N channel refocusing π pulse. (A) Selective magnetization transfer is performed by SAMPI4 [9,25]. (B) Magnetization transfer is performed by WIM. WIM-24 follows the same phase cycle as previously described [46], and the φ pulse is cycled between Y and –Y, and in combination with the preceding Y pulse, it cancels the spin-locked component [46]. In our experience, WIM provides higher sensitivity for magnetization transfer, while SAMPI4 provides better dipolar coupling results.