We report a stable, high-power, high-repetition-rate, picosecond ultraviolet (UV) source at 355 nm based on singlepass sum-frequency generation of a mode-locked Yb-fiber laser at 1064 nm in the nonlinear crystal BiB 3 O 6 . By performing single-pass second-harmonic generation (SHG) in a 30-mm-long LiB 3 O 5 crystal, up to 9.1 W of average green power at 532 nm is obtained at a single-pass SHG efficiency of 54%. The generated green pulses have a duration of 16.2 ps at a repetition rate of 79.5 MHz, with a passive power stability better than 0.5% rms and a pointing stability <12 μrad over 1 h, in high beam quality. The green radiation is then sum-frequency-mixed with the fundamental in a 10-mm-long BiB 3 O 6 crystal, providing as much as 1.2 W of average UV power, at an infrared-to-UV conversion efficiency of 7.2%, with a passive power stability better than 0.4% rms over 3 h and a pointing stability <45 μrad over 1 h, in TEM 00 spatial profile. . For many years, the development of such ultrafast sources has relied almost entirely on nonlinear optical techniques based on third (∼355 nm) and fourth (∼266 nm) harmonic generation of widely established mode-locked Nd/Yb-doped solid-state lasers at ∼1064 nm. The rapid advances in fiber laser technology in recent years, however, have paved the way for the replacement of bulky, water-cooled, mode-locked solidstate lasers with compact, air-cooled, ultrafast Yb-fiber lasers at ∼1064 nm. With the availability of multiwatt average powers, and the potential for further power scaling, the exploitation of mode-locked Yb-fiber lasers thus offers great promise for the realization of efficient and high-power picosecond UV sources in more practical designs by deploying third and fourth harmonic generation schemes. On the other hand, to fully exploit the advantages of fiber lasers with regard to a compact architecture, simplicity, and portability, it would also be crucial to deploy the most direct nonlinear techniques for UV generation in order to preserve those important merits. To this end, single-pass conversion schemes offer the most effective approach to achieve this goal. We have already verified the viability of such single-pass schemes in combination with continuous-wave (cw) and modelocked Yb-fiber lasers for efficient generation of highpower cw radiation in the green and UV [4], and high-average-power picosecond pulses in the green [5]. Recently, a fiber-based femtosecond green source was also demonstrated [6]. At the same time, a critical factor in the attainment of the highest nonlinear conversion efficiency and output power is the choice of suitable nonlinear materials. For UV generation, this choice is particularly limited and is especially challenging when low-intensity picosecond pulses at high repetition rates are involved. In addition to a wide transparency in the UV, of paramount importance are a sufficiently high effective nonlinearity, low spatial walk-off, high optical damage threshold, low transmission loss, and high optical quality, as well as chemical and the...