@article{grigoriev_chiral_properties_2013, author={Grigoriev, S.V. and Potapova, N.M. and Siegfried, S.-A. and Dyadkin, V.A. and Moskvin, E.V. and Dmitriev, V. and Menzel, D. and Dewhurst, C.D. and Chernyshov, D. and Sadykov, R.A. and Formicheva, L.N. and Tsvyashchenko, A.V.}, title={Chiral Properties of Structure and Magnetism in Mn 1-x Fe x Ge Compounds: When the Left and the Right are Fighting, Who Wins?}, year={2013}, journal = {Physical Review Letters}, volume = {110}, number = {20}, pages = {207201}, doi = {http://dx.doi.org/10.1103/PhysRevLett.110.207201}, abstract = {Magnetic susceptibility measurements have shown that the compounds Mn 1-x Fe x Ge are magnetically ordered through the whole range of concentrations x=[0.0,1.0] . Small-angle neutron scattering reveals the helical nature of the spin structure with a wave vector, which changes from its maximum (|k|=2.3  nm −1 ) for pure MnGe, through its minimum (|k|→0 ) at x c ≈0.75 , to the value of |k|=0.09  nm −1 for pure FeGe. The macroscopic magnetic measurements confirm the ferromagnetic nature of the compound with x=x c . The observed transformation of the helix structure to the ferromagnet at x=x c is explained by different signs of chirality for the compounds with x>x c and x