Current induced by a tilted magnetic field in phosphorene under terahertz laser radiation

TL;DR

This paper explores how a tilted magnetic field influences cyclotron resonance, AC currents, and second harmonic generation in phosphorene under terahertz laser radiation, revealing multiple resonance conditions and polarization effects.

Contribution

It provides a detailed analysis of cyclotron resonances and current behaviors in phosphorene with a tilted magnetic field, highlighting novel resonance conditions and polarization dependencies.

Findings

Cyclotron resonances depend on the magnetic field and effective masses.

Current magnitude varies with radiation polarization and magnetic field orientation.

Resonance conditions are identified for different harmonic generations.

Abstract

In this study, we investigate the cyclotron resonance effect in the first-order AC current, magnetic ratchet effect, and second harmonic generation in phosphorene in the presence of a steady tilted magnetic field and under THz laser radiation. We establish that various cyclotron resonances exist in the deduced currents based on the angular frequency of the incoming light. These resonances are dependent on the $\omega_{c_{+}}$ value, a function of the carrier charge, the perpendicular magnetic field, and the effective masses along the armchair or zigzag edges. We discuss the direction and the magnitude of the deduced currents for various radiation polarizations. We compare the results with a zero perpendicular magnetic field. Cyclotron resonance for the first order AC current occurs at $\omega= \pm \omega_{c_{+}}$. The deduced current declines if the perpendicular magnetic field is zero. Meanwhile, for the ratchet current, cyclotron resonances occur at $\omega= \pm \omega_{c_{+}}$, $\omega= \pm 2\omega_{c_{+}}$, and radiation helicity affects the deduced current for circularly polarized light. Cyclotron resonance for the second harmonic generation current occurs at $\omega= \pm \omega_{c_{+}}$, $\omega= \pm 2 \omega_{c_{+}}$ and $\omega= \pm \omega_{c_{+}}/2 $ and the current is stronger compared to the case with no perpendicular magnetic field. As the magnetic field rotates in the plane of anisotropic phosphorene, separate directions are predicted for the second harmonic generation--related current. It is noteworthy that the magnitude of the ratchet and second harmonic generation current are within the same range and comparable to the magnetic ratchet current in monolayer graphene, $\mu A / cm$.