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A neutron reflector is any material that reflects neutrons. Usually, this term refers to the elastic scattering rather than to a specular reflection. This reflector (scatterer) may be graphite, beryllium, or other materials. A neutron reflector can make an otherwise subcritical mass of fissile material critical, or increase the amount of nuclear fission that a critical or supercritical mass will undergo.
In a uranium graphite chain reacting pile the critical size may be considerably reduced by surrounding the pile with a layer of graphite, since such an envelope reflects many neutrons back into the pile. A similar envelope can be used to reduce the critical size of a nuclear weapon, but here the envelope has an additional role: its very inertia delays the expansion of the reacting material. For this reason such an envelope is often called a tamper. As has already been remarked, the weapon tends to fly to bits as the reaction proceeds and this tends to stop the reaction, so the use of a tamper makes for a longer lasting, more energetic, and more efficient explosion. The most effective tamper is the one having the highest density; high tensile strength turns out to be unimportant because no material will hold together under the extreme pressures of a nuclear weapon. Coincidently, high density materials are excellent neutron reflectors. This makes them doubly suitable for nuclear weapons.
While the effect of a tamper is to increase the efficiency - both by reflecting neutrons and by delaying the expansion of the bomb, the effect on the critical mass is not as great as on the efficiency. The reason for this is that the process of reflection is relatively time consuming and may not occur extensively before the chain reaction is terminated.
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