Nonplanar Ring Oscillators
A nonplanar ring oscillator is a laser oscillator with a special monolithic design, which is very stable, compact and rugged. The resonator of an NPRO laser (Figure 1) consists of a single laser crystal (typically made of Nd:YAG) within which the laser light circulates. On one of the internal surfaces (the front face, which can have a slightly convex shape), there is a partially reflective dielectric mirror coating which is highly transmissive for the pump light (blue beam) and serves as the output coupler mirror of the resonator. On all other internal surfaces, total internal reflection occurs.
Such lasers have originally been called MISERs = monolithic isolated single-mode end-pumped rings, but later the term NPRO = nonplanar ring oscillator became more common.
An important detail is that the ring resonator of an NPRO is nonplanar. This causes a slight rotation of the polarization direction in each round-trip. If a small magnet is attached to the laser crystal, its magnetic field can cause an additional polarization rotation via the Faraday effect. For one of the two oscillation directions, the two polarization rotations partly cancel, leading to a lower optical loss when the beam hits the output coupler face of the crystal (because the coating has a slightly polarization-dependent reflectivity). The other oscillation direction leads to a higher loss and is thus firmly suppressed. In this way, one easily obtains unidirectional operation, thus avoiding any standing-wave patterns (except very near to the reflection points), which would cause spatial hole burning. For this reason, with nonplanar ring oscillators one easily obtains stable single-frequency operation.
Most NPROs are made of Nd:YAG. It is possible, however, to use other materials, such as Yb:YAG. In that case, reabsorption losses in unpumped regions can be eliminated by using a composite laser crystal, consisting of Yb:YAG and undoped YAG pieces which are bonded to each other.
Given that the round-trip length is short (typically between a few centimeters and 10 cm), the NPRO cavity has a relatively large free spectral range, which allows for continuous (mode-hope free) frequency tuning over several gigahertz. Tuning can be achieved with a piezoelectric transducer pressing on the crystal, by changing the crystal temperature with a Peltier element, or by adjusting the pump power. There have also been nonplanar ring lasers containing an electro-optic crystal for tuning.
Due to the stable mechanical setup, the low optical losses of the laser resonator and the low noise of a laser diode as pump source, the laser noise of an NPRO can be very small. Typical linewidths are in the region of a few kilohertz. Output powers up to several watts have been achieved. NPROs are often used as master lasers for high-power single-frequency MOPA devices.
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|||T. J. Kane and R. L. Byer, “Monolithic, unidirectional single-mode ring laser”, Opt. Lett. 10 (2), 65 (1985), doi:10.1364/OL.10.000065|
|||A. C. Nilsson et al., “Eigenpolarization theory of monolithic nonplanar ring oscillators”, IEEE J. Quantum Electron. 25 (4), 767 (1989), doi:10.1109/3.17343|
|||N. M. Sampas et al., “Long-term stability of two diode-laser-pumped nonplanar ring lasers independently stabilized to two Fabry–Pérot interferometers”, Opt. Lett. 18 (12), 947 (1993), doi:10.1364/OL.18.000947|
|||C. C. Harb et al., “Suppression of the intensity noise in a diode-pumped neodymium:YAG nonplanar ring laser”, IEEE J. Quantum Electron. 30 (12), 2907 (1994), doi:10.1109/3.362718|
|||I. Freitag et al., “Power scaling of diode-pumped monolithic Nd:YAG lasers to output powers of several watts”, Opt. Commun. 115, 511 (1995), doi:10.1016/0030-4018(95)00020-9|
|||E. J. Zang, “Single-frequency 1.25 W monolithic lasers at 1123 nm”, Opt. Lett. 32 (3), 250 (2007), doi:10.1364/OL.32.000250|
|||B. Yao et al., “7.3 W of single-frequency output power at 2.09 μm from an Ho:YAG monolithic nonplanar ring laser”, Opt. Lett. 33 (18), 2161 (2008), doi:10.1364/OL.33.002161|
See also: lasers, ring lasers, ring resonators, single-frequency operation, single-frequency lasers, microchip lasers
and other articles in the categories optical resonators, laser devices and laser physics