JETP Letters: issues online

$For an anisotropic layered superconductor we have calculated the magnetization ve absolute value И and orientation of the external magnetic field. It displays a cusp at a field Μ = Χι(θ), where θ is the angle between the field and the layers, and a maximum at some characteristic field X = #s(0) α (sini)-1 in agreement with the experimental meaeurments by Zavaritsky N.V. and Zavaritsky V.N. We predict the existence of an intermediate critical field Μ = Μ3{θ) ос (sinfl)-1 at which the perpendicular to the layers component of the magnetic induction first penetrates the sample. The magnetic susceptibility χ = дМ/дХ has a jump at N = The jump is very small at в > 7_1, where 7 is the anisotropy coefficient. In this range of angles one can observe a cusp on a graph of χ vs )( at К = U^This prediction of theory is in good agreement with the experiment a.$

For an anisotropic layered superconductor we have calculated the magnetization ve absolute value И and orientation of the external magnetic field. It displays a cusp at a field Μ = Χι(θ), where θ is the angle between the field and the layers, and a maximum at some characteristic field X = #_s(0) α (sini)^-1 in agreement with the experimental meaeurments by Zavaritsky N.V. and Zavaritsky V.N. We predict the existence of an intermediate critical field Μ = Μ₃{θ) ос (sinfl)^-1at which the perpendicular to the layers component of the magnetic induction first penetrates the sample. The magnetic susceptibility χ = дМ/дХ has a jump at N = The jump is very small at в > 7^_1, where 7 is the anisotropy coefficient. In this range of angles one can observe a cusp on a graph of χ vs )( at К = U^This prediction of theory is in good agreement with the experiment ^a.