We experimentally investigate the limits to 800 nm-to-terahertz (THz) energy conversion in lithium niobate at room temperature driven by amplified Ti:Sapphire laser pulses with tilted-pulse-front. The influence of the pump central wavelength, pulse duration, and fluence on THz generation is studied. We achieved a high peak efficiency of 0.12% using transform limited 150 fs pulses and observed saturation of the optical to THz conversion efficiency at a fluence of 15 mJ/cm 2 . We experimentally identify two main limitations for the scaling of optical-to-THz conversion efficiencies: (i) the large spectral broadening of the optical pump spectrum in combination with large angular dispersion of the tilted-pulse-front and (ii) free-carrier absorption of THz radiation due to multi-photon absorption of the 800 nm radiation. Strong-field terahertz (THz) sources hold promise for enabling myriads of novel applications. They possess intense electric and magnetic fields at frequencies which are particularly amenable to studies of condensed matter dynamics [1][2][3], manipulation of molecules [4], highharmonic generation (HHG) [5], and compact chargedparticle acceleration [6][7], among others. Therefore, there is a great need for the development of robust and efficient strong-field THz sources.These sources are predominantly accelerator-based facilities (delivering up to 100 µJ THz energy) [8,9] or ultrafast laser-based table-top systems [10]. Laboratory scale systems are of particular interest due to accessibility and relatively low cost. In this category, laser-induced air/gas plasmas (delivering up to 5 µJ THz energy) [11] and optical rectification (OR) of infrared (IR) pulses in nonlinear optical crystals (delivering up to 0.4 mJ THz energy) [12] have emerged as the most common methods of all THz generation modalities. The highest optical-toTHz conversion efficiencies (henceforth referred to as conversion efficiency) in excess of 1% at room temperature have been achieved by OR employing angularly dispersed femtosecond IR pump pulses in lithium niobate [13,14]. As a result, these systems are especially relevant to generating mJ-level THz pulses [12]. In this approach, angular dispersion is introduced to compensate for the large difference in refractive indices between IR and THz frequencies by forming a tilted-pulse-front. The generated THz then propagates perpendicular to this tilted-pulsefront and phase matching is achieved in a non-collinear configuration. OR systems based on lithium niobate are powered predominantly by sources in the 1 µm and 800 nm wavelength regions. While the former yields much higher conversion efficiencies, today, 800 nm sources based on Ti:Sapphire systems prevail in ultrafast laser technology as the most accessible and widely employed sources. Consequently, exploring the limits to achievable conversion efficiency is a great value in the pursuit of accessible high-energy THz sources.In this paper we extensively investigate the limits of conversion efficiency with 800 nm systems through a systemati...