Abstract
We suggest a theory of the Field-Induced Charge-Density-Wave (FICDW) phases, generated by high magnetic fields in quasi-low-dimensional conductors. We demonstrate that, in layered quasi-one-dimensional conductors, the corresponding critical magnetic fields ratios are universal and do not depend on any fitting parameter. In particular, we find that , where is a critical field of a phase transition between the FICDW phases with numbers and . The suggested theory is in very good qualitative and quantitative agreements with the existing experimental data in -(ET)KHg(SCN) material.
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