Lawrence Livermore National Laboratory

Schematic layout of NIF’s final optics assembly (FOA). The suite of optics for one beamline is on the right.

The final optics assemblies (FOAs) are the last element of the main laser system and the first of the target area systems. Each FOA contains four integrated optics modules (IOMs) that incorporate beam conditioning, frequency conversion, focusing, diagnostic sampling, and debris shielding capabilities into a single compact assembly. These optics are shown in the figure at right. The same mechanical, optical, and beam control components that are used in the FOA at the target chamber are reproduced for a single beamline in the precision diagnostic system.

The FOAs mount to the NIF target chamber and house the final set of optics for four NIF beamlines as line replaceable units; each optic can be individually replaced as required. NIF’s 192 beamlines connect to the target chamber, in groups of four, through the 48 FOAs. The FOAs are symmetrically distributed around the upper and lower hemispheres of the target chamber so that the laser beams are optimally located to provide the proper orientation as they are directed toward the target. Adjustments of the final turning mirrors allow pointing the focused beams to different locations near the center of the target chamber (+/- 3 cm) to accommodate a variety of experiments.

Final Optics Assemblies Final optics assemblies attached to the lower hemisphere of the NIF target chamber (blue).

One of the chief functions of the FOAs is to change the laser light to a shorter wavelength. NIF’s neodymium glass lasers generate light at a fundamental wavelength of about 1,053 nanometers (one omega, or 1ω) in the infrared region. Inertial confinement fusion targets, however, perform more efficiently when they are driven with 351-nm ultraviolet light (3ω). To change the laser light frequency, the 1ω light passes through two nonlinear crystal plates made of potassium dihydrogen phosphate (KDP), the same type of crystal used in NIF’s Pockels cell optical switch. The first plate converts two-thirds of the 1,053-nanometer radiation to the 527-nm second harmonic (2ω) wavelength, which is visible green light. The second crystal then mixes that radiation with the remaining infrared light to produce 351-nm ultraviolet radiation at the third harmonic (3ω).

Other functions of the FOAs are also critical to achieving the required laser performance for use in target experiments. In all, the FOAs provide a vacuum barrier for the target chamber, convert 1ω to 3ω light, focus the 3ω light to target center, allow for beam smoothing, allow for 3ω power measurement, and provide a protective shield from target debris.

Replacement of each final optic is done using specialized clean cassettes attached to the IOM hatches.