The Reflection Asymmetric Shell Model (RASM) has been established by means of the variational procedure and the projection method to describe the high spin states in octupole deformed nuclei. Recently, the model has been generated to include the triaxiali The Reflection Asymmetric Shell Model (RASM) has been established by means of the variational procedure and the projection method to describe the high spin states in octupole deformed nuclei. Recently, the model has been generated to include the triaxiali