We report on tunable terahertz resonant detection of two 1.55 µm cw-lasers beating by plasma waves in AlGaAs/InGaAs/InP high-electron-mobility transistor. We show that the fundamental plasma resonant frequency and its odd harmonics can be tuned with the applied gate-voltage in the range 75-490 GHz. The observed frequency dependence on gate-bias is found to be in good agreement with the theoretical plasma waves dispersion law.PACS numbers: 85.30. Tv, 52.35.-g, 61.80.Ba, 2006 Operating optic-to-electronic data conversion at the terahertz (THz) frequency range is one of the most promising issue of optoelectronic devices. Recently, experimental studies on the plasma resonant detection in high electron mobility transistors (HEMTs) and in a single and a double quantum well field effect transistors (FETs) have been published [1,2,3,4,5,6]. For submicron gate-lengths, fundamental plasma frequencies reach the THz range [7]. THz detection by plasma waves is easily tunable by changing the gate-voltage. Spectral profiles of THz plasma waves resonances were first reported by T. Otsuji et al., the HEMT being excited by means of interband photoexcitation using the differencefrequency component of a photomixed laser beam [8].With a similar experiment, we investigate in this letter the plasma waves resonances excited in the channel of HEMTs by the beating of two cw-lasers. We show that the plasma resonant frequencies follow the square-root dependence versus applied gate-voltage as initiallypredicted by Dyakonov-Shur theory [7].Experiments were performed using an AlGaAs/InGaAs/InP HEMT with gate-length L g = 800 nm and a threshold voltage of V th = -150 mV extracted from the transfer characteristics (inset (a) of The whole HEMT structure is transparent to the incident radiation excepted the InGaAs-channel where the interband photoexcitation occurs. By using a tunable optical beating this photoexcitation is modulated over a large frequency range. Two commercially-available cw-lasers sources centered at λ 1 = 1543 nm and λ 2 = 1545 nm are used. Each powerful laser (≈ 20 mW) can be tuned over a range of ≈ ± 1 nm by varying the temperature. Their mixing produces a tunable optical beating from 0 to 600 GHz. The collimated beams are mechanically chopped at 120 Hz and focused onto the