The magnetization of the triangular antiferromagnet RbFeCl 3 has been measured as a function of magnetic field and temperature in the applied field parallel to the a -axis. It is found that a new phase exists between the commensurate up-up-down phase and the incommensurate fan phase. It is suggested that the new phase is a commensurate phase with a coplanar structure which is stabilized by the quantum fluctuation in magnetic fields.
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Ono et al. (1999) studied this question.
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