Hohlraum
In radiation thermodynamics, a hohlraum is a cavity whose walls are in radiative equilibrium with the radiant energy within the cavity. First proposed by Gustav Kirchhoff in 1860 and used in the study of black-body radiation, this idealized cavity can be approximated in practice by a hollow container of any opaque material. The radiation escaping through a small perforation in the wall of such a container will be a good approximation of black-body radiation at the temperature of the interior of the container. Indeed, a hohlraum can even be constructed from cardboard, as shown by Purcell's Black Body Box, a hohlraum demonstrator.
In spectroscopy, the Hohlraum effect occurs when an object achieves thermodynamic equilibrium with an enclosing hohlraum. As a consequence of Kirchhoff’s law, everything optically blends, and the contrast between the walls and the object effectively disappears.
Applications
Hohlraums are used in high energy density physics and inertial confinement fusion experiments to convert laser energy to thermal X-rays for imploding capsules, heating targets, and generating thermal radiation waves. They may also be used in nuclear weapon designs.Inertial confinement fusion
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. Inside the hohlraum is a fuel capsule containing deuterium and tritium fuel. A frozen layer of D-T ice adheres to the inside of the fuel capsule.The fuel capsule wall is fabricated using light elements such as plastic, beryllium, or high-density carbon, i.e. diamond. The outer portion of the 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 of the fuel capsule implodes, causing the D-T fuel to be supercompressed, activating a fusion reaction.
The radiation source is pointed at the interior of the hohlraum rather than at the fuel capsule itself. The hohlraum absorbs and re-radiates the energy as X-rays, a process known as indirect drive. The advantage of 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 of this approach is that low-mode asymmetries are more complex to control. It is essential to be able to control both high-mode and low-mode asymmetries to achieve a uniform implosion.
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, imperfections are to be carefully avoided, so surface finishing is critical, as during ICF laser shots, due to the intense pressure and temperature, results are highly susceptible to hohlraum texture roughness. The fuel 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 a diameter of less than 5 microns to inject D-T gas into the capsule.
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 maintaining adequate X-ray symmetry proved difficult 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 significant 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.