“…Since the occurrence of weak ferromagnetism requires an additional antisymmetric Dzyaloshinsky-Moriya-type exchange interaction term in otherwise symmetric Cu-O-Cu superexchange interaction, it is speculated that a slight oxygen distortion in the CuO 2 layer is necessary for Cu WF/CAF order in the Gd 2 CuO 4 -type cuprates. 2,[5][6][7][8][9][10][11][12][13][14] Although single-crystal x-ray diffraction on Gd 2 CuO 4 gives a good fitting using the tetragonal TЈ-phase space group 14/mmm with Cu͑0,0,0͒ and oxygen O͑1͒͑0, 1 2 ,0͒ in CuO 2 layer formed a perfect square-planar arrangement, 1 large plane oxygen mean-square displacement U eq of 2.5 Å 2 at room temperature indicates that stable oxygen position may not be in the ideal ͑0, 1 2 ,0͒ sites. Single-crystal neutron diffraction of 158 Gd 2 CuO 4 based on TЈ-phase structure shows that Cu moments order below T N ͑Cu͒ to a basically AF structure with the propagation vector kϭ( 1 2 , 1 2 ,0) and the Cu moments are oriented parallel to the ͓110͔ direction of the tetragonal basal plane.…”