Fig. 4From: Plasma frequency demand for mode conversion processes from slow Z-mode to LO-mode waves in an inhomogeneous plasmaVariation of wave normal angle \(\theta\) as a function of \({{\omega_{p} } \mathord{\left/ {\vphantom {{\omega_{p} } {\omega_{c} }}} \right. \kern-0pt} {\omega_{c} }}\) for the incident wave with \({\omega \mathord{\left/ {\vphantom {\omega {\omega_{c} }}} \right. \kern-0pt} {\omega_{c} }} = 2.1\). Blue curves are under the condition that Eq. (4) can be satisfied and red curves are under the condition that Eq. (4) cannot be satisfied. RP indicates the return point where the plasma frequency becomes maximum along the ray-path in the inhomogeneous mediumBack to article page