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. 2024 Jun 11;26(29):19630–19645. doi: 10.1039/d4cp01785d

Fig. 9. Comparison of the measured 3He scattering from Cu(111) signals (black solid line) with the calculated signals (red dashed line) for B1 scans when B2 = 11.2 gauss metre at a nozzle temperature of 40 K (top row), B1 scans when B2 = −11.2 gauss metre at a nozzle temperature of 60 K (second row), B2 scans when B1 = −11.2 gauss metre at a nozzle temperature of 40 K (third row) and B2 scans when B1 = 11.2 gauss metre at a nozzle temperature of 60 K (bottom row). Each column magnifies a different echo, with the first and third showing either the parallel echo (B1 = B2, the largest amplitude) or anti-parallel echo (B1 = −B2, the smallest amplitude), and the middle column showing the X′ echo in the B1 scans (top two rows) or X echo in the B2 scans (bottom two rows).

Fig. 9