The indirect drive approach to inertial confinement fusion is as follows; the fusion fuel capsule is held inside a cylindrical hohlraum. The hohlraum body is manufactured using a high-Z element, usually gold or uranium. The hohlraum walls must have surface roughness less than 1 micron, and hence accurate machining is required during fabrication. Any imperfection of the hohlraum wall during fabrication will cause uneven and non-symmetrical compression of the fuel capsule inside the hohlraum during inertial confinement fusion. Hence surface finishing is extremely important, as during ICF laser shots, due to intense pressure and temperature, results are highly susceptible to hohlraum texture roughness. Therefore imperfection during hohlraum fabrication is to be carefully prevented. Inside the hohlraum is a fuel capsule containing deuterium and tritium fuel. A frozen layer of D-T ice adheres inside the fuel capsule. The fuel capsule wall is synthesized using light elements . The outer portion of fuel capsule explodes outward when ablated by the x-rays produced by the hohlraum wall upon irradiation by lasers. Due to Newton's third law, the inner portion the fuel capsule implodes, causing the D-T fuel to be supercompressed activating fusion reaction. The capsule must be precisely spherical, with texture roughness less than one nanometer, for fusion ignition to start. Otherwise instability will cause fusion to fizzle. The fuel capsule contains a small fill hole with less than 5 microns diameter, to inject the capsule with D-T gas. Depending on hohlraum design, during ICF laser shots, various parameters like shock timing, fuel capsule implosion shape, implosion velocity, and ratio of the cold fuel to the hot fuel core are measured. The radiation source is pointed at the interior of the hohlraum rather than at the capsule itself. The hohlraum absorbs and re-radiates the energy as X-rays, a process known as indirect drive. The advantage to this approach, compared to direct drive, is that high mode structures from the laser spot are smoothed out when the energy is re-radiated from the hohlraum walls. The disadvantage to this approach is that low mode asymmetries are harder to control. It is important to be able to control both high mode and low mode asymmetries to achieve a uniform implosion. The X-ray intensity around the capsule must be very symmetrical to avoid hydrodynamic instabilities during compression. Earlier designs had radiators at the ends of the hohlraum, but it proved difficult to maintain adequate X-ray symmetry with this geometry. By the end of the 1990s, target physicists developed a new family of designs in which the ion beams are absorbed in the hohlraum walls, so that X-rays are radiated from a large fraction of the solid angle surrounding the capsule. With a judicious choice of absorbing materials, this arrangement, referred to as a "distributed-radiator" target, gives better X-ray symmetry and target gain in simulations than earlier designs.
The term hohlraum is also used to describe the casing of a thermonuclear bomb following the Teller-Ulam design. The casing's purpose is to contain and focus the energy of the primary stage in order to implode the secondary stage.
