Spectral and temporal properties of a scanning injection-seeded b-barium borate optical parametric oscillator pumped by the third harmonic of a 10-Hz Nd:YAG laser have been studied. The seed source was a cw diode laser with a wavelength of 830 nm tunable over a range of 50 GHz. We measured the bandwidth of the seeded optical parameter oscillator, using a two-photon resonance in barium and a Fabry -Perotétalon, to be approximately 400 MHz for pump power levels more than two times above threshold. This is ϳ2 times the Fourier-transform-limited bandwidth. At lower pump powers the bandwidth was smaller.A solid-state optical parametric oscillator (OPO) is an attractive source of coherent radiation that is tunable over a broad wavelength range. This has been recognized since the first demonstration of the OPO in 1965, 1 but at that time high-quality and efficient nonlinear crystals were not available, hampering widespread use of OPO's in, for example, spectroscopic applications. Recently this situation changed dramatically because of the availability of new materials such as b-barium borate (BBO), lithium triborate, and potassium titanyl phosphate with large nonlinear coefficients and high damage thresholds. Our main interest is the development of nanosecond OPO's pumped by the second and third harmonics of a Nd:YAG laser for spectroscopic applications. A free-running OPO does not provide the required narrow-band radiation; however, the bandwidth can be reduced considerably by use of intracavity elements such as gratings 2 andétalons 3 or by injection seeding with a narrow-band laser on either the signal or the idler wavelength. 4 When the bandwidth of the pump laser is sufficiently small, the energy conservation condition for the OPO ensures that the signal and the idler have comparable bandwidths. Hence, if one of these waves is constrained to be narrow band, then the other will be likewise constrained. When the bandwidth of the seed laser is also small, the bandwidth of the seeded OPO (both signal and idler) may in principle be reduced to the Fourier-transform limit.In this Letter we report the operation of a BBO OPO seeded with a cw diode laser. The experimental setup is shown in Fig. 1. We use a type I BBO crystal (6 mm 3 6 mm 3 12 mm) cut at an angle of Q 30 ± . It is pumped by the third harmonic (355 nm) of a Q-switched Nd:YAG laser (Spectra-Physics GCR-3; repetition rate, 10 Hz; injection seeded for operation in a single axial mode; bandwidth, ϳ90 MHz). The pump beam has a diameter of 7 mm and a pulse duration of 5 ns. The beam diameter of the Nd : YAG laser is reduced by a factor of 2 with a telescope.The OPO cavity has a three-plane-mirror ring configuration and is 10 cm long, preventing the backreflection of pump light from the mirrors into the pump laser. This setup is also advantageous for injection-seeding experiments. The three identical mirrors have high reflectance on the idler wavelength (90%), whereas the reflectance for the signal wavelength is 10%. The transmission for the pump wavelength is .90%....