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Figure 7
Rocking curves of [{}^3P_{\rm m}^{ \langle n \rangle }] and 3Pt + 3Plt from the third crystal. Solid squares shows [{}^3P_{\rm m}^{ \langle 1 \rangle }], open circles [{}^3P_{\rm m}^{ \langle 2 \rangle }], solid circles [{}^3P_{\rm m}^{ \langle 3 \rangle }] and open squares [{}^3P_{\rm m}^{ \langle 4 \rangle }]. The rocking curves of 3Pt + 3Plt (left) were measured simultaneously with the curve of [{}^3P_{\rm m}^{ \langle n \rangle }] with n = 1, 2, 3 and 4. The peak angles of [{}^3P_{\rm m}^{ \langle n \rangle }] for n = 1, 2, 3 and 4 correspond to the angles of the refracted beam [{{\bf{S}}_{\rm m1}}] in Fig. 1[link](b). The shoulder structures of [{}^3P_{\rm m}^{ \langle n \rangle }] on the high-angle side are probably caused by the component of the refracted beam [{{\bf{S}}_{\rm m2}}]

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 47| Part 4| August 2014| Pages 1267-1272
https://doi.org/10.1107/S1600576714012114
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