Demonstration of Broadband Non-Resonant Time-Crystal Amplification in Microwaves

TL;DR

This paper demonstrates broadband non-resonant amplification in a microwave photonic time crystal, overcoming losses and finite-size effects to achieve stable gain over a wide frequency range.

Contribution

It presents the first experimental realization of a broadband microwave photonic time crystal with stable amplification, using a time-modulated capacitor circuit with optical control.

Findings

Achieved a peak gain of 3.8 dB over 65 MHz bandwidth.

Observed a narrow parametric resonance with 4.8 dB gain.

Demonstrated that finite-size and loss effects modify the ideal gain profile.

Abstract

We report an optically modulated experimental realization of a photonic time crystal (PTC) in the microwave regime, demonstrating for the first time that the PTC exponential growth can overcome losses and finite-size constraints of a practical spatio-temporal system and yield stable positive terminal gain over a continuous broadband frequency range. The developed experimental platform is a purely time-modulated capacitor (TMC) microwave circuit based on a microstrip transmission line, in which synchronized optical modulation of reverse-biased photodiodes generates strong (94.5 %) temporal modulation of the effective capacitance at 200 MHz. Broadband amplification consistent with a momentum band gap (MBG), a defining signature of photonic time-crystal physics, is observed, with a peak gain of 3.8 dB over a 65 MHz bandwidth. In addition, a narrow parametric resonance appears at the center of the band gap, reaching 4.8 dB. This sharp peak is associated with the spatial inhomogeneities of the lumped-element realization, while the corresponding homogeneous distributed system retains the Floquet-mode structure of a photonic time crystal. We show that finite microwave TMC implementations inherit the defining physics of PTCs, including phase-invariant non-resonant amplification and slow-light behavior inside the momentum band gap, while finite-size and loss mechanisms transform the ideal semicircular PTC gain profile into a continuous asymmetric non-Lorentzian gain band characterized by a Pearson type IV distribution.