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Fig. 2 (Color online) Resonant elastic soft x­ray scattering at theCanadian Light Source. The endstation has been already in­stalled, and the three remaining chambers (transfer cham­ber, sample characterization chamber, and molecular beam
epitaxy chamber) will be also connected.

118  úËõ March 2013 Vol.26 No.2
(C) 2013 The Japanese Society for Synchrotron Radiation ResearchúËõj3.

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To compare lineshapes, all data in the panels (a) and (b)have been normalized to each spectrum area, shown at therespective panels (c) and (d) as a function of photon ener­
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Fig. 4©ç­é¥»ðp¢éªC}`tFCbN¨¿ÍdCªÉÆ¥»Ì¼ûð¯ÉÂ©çÅéBpãÍC¥êðp¢¸dêÌÝÅ¥»ð§ä·é±ÆC³çÉ±êðº·ÅÀ»·é±ÆªÁÉå«ÈÚWÆÈÁÄ¢éBÅßC }`t FCbN «ð¦·y uXJCg ^ÌYMnO3 Ìì»ªñ³êCå«ÈdCªÉðÂ±(Color online) Temperature dependence of the (0 qb 0) (qb`0.5) magnetic peaks (a) taken at hn643.1 eV(Mn 2p3/2¨3d absorption edge) and the (0 1 0) lattice­distortion peaks (b) taken at hn12 keV.

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cycloidal (b) antiferromagnetic states. (a) Spins align an­tiparallel to each other, resulting in a large lattice strain andlarge electric polarization. (b) Spins align helically along theb­axis, resulting in small electric polarization.

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