Soon after Franken et al. observed second-harmonic generation^[1], Kingston et al. proposed an optical parametric oscillator in 1962^[2,3], and then Wang and Racetle first, to the best of our knowledge, observed parametric gain of the laser in NH4H2PO4 (ADP) crystals in 1965^[4]. Subsequent research and further development of optical parametric amplification (OPA) have received significant attention due to its ability to amplify weak signals with high and ultra-broadband gain, meanwhile, generating the difference frequency light (i.e., idler beam). This technique has been applied in various areas such as strong-field physics, tunable infrared-laser generation, and noiseless image amplification^[5–9]. The emergence of structured light represented by beams carrying orbital angular momentum (OAM) renewed broad research interest^[10–14]. Beyond the OAM, structured light, in principle, can be extended to all degrees of freedom and dimensions, which has revived many areas ranging from classical to quantum light and fundamental physics to advanced photonic techniques^[15–19]. Structured light can typically be generated by low-peak-power devices such as liquid-crystal spatial light modulators (SLMs)^[20], digital micromirror devices^[21–23], q-plates^[24], and other spin-orbit approaches^[25–27]. The need for structured light demonstrations at higher powers for industrial applications has remained an open challenge^[10]. OPA is an alternative method to obtain high-power structured light. The OPA of OAM-carrying beams and the transformation of OAM were studied both theoretically and experimentally^[28–30]. Polarization-insensitive OPA of radially polarized femtosecond pulses was also successfully achieved with high gain^[31].