What is the spectrum of a nuclear bomb in a vacuum? This question about 'nukes in space' mentions that the two forms of energy released from a nuclear bomb come from neutrons and photons (the latter about 104 times the former).
It's mentioned that the photons are in the form of X-rays, but what is the actual spectrum of the light emitted? How much of the light comes from 


*

*the fission (assume pure-fission bomb for simplicity) where 239Pu is split into a mish-mash of lighter elements (is this energy quantized, i.e. has "peaks"?)

*black-body emission (the results being heated to 10x K; is this continuous or does strange stuff happen at very high temperatures?)

*extremely short-lived fission products

 A: I worked on a program two decades ago where we were to determine if nations "XYZ" were building nuclear weapons based on intelligence "ABC." Before I did this I took a DOE course that amounted to intermediate level (210) nuclear weapons. A lot of data on this is classified, and one needs CWDI Q-clearance to know this stuff. A lot of effort has gone into measuring just these physical parameters. After the 1963 nuclear test treaty restricted tests to underground (a really good thing) these tests used detectors and cables that measured these things. The bomb under ground would register data on a detector that is vaporized and the data would travel up transmission lines ahead to the destruction. A lot of this data collected is highly classified.
One can get a rule of thumb understanding of things. The temperature in the immediate environment of a nuclear bomb is about $5\times 10^7$K. Using Wein's law $\nu_{max}~\simeq~(2.9/hc)kT$ for the frequency at the black body peak for this temperature $\nu~=~3.3\times 10^{18}$Hz and equivalently $\lambda~=~9\times 10^{-11}m$. We can also calculate the energy $E~=~h\nu$ that is $12$KeV. This in the X-ray range of energy. If you were to place a photon detector in space to measure a nuclear burst this would be about where the peak of the EM spectrum would be.
These photons are are secondaries after interacting with the materials of the bomb. The initial nuclear induced photons are at higher energy. The nuclear process does not primarily generate photons, which are generated by QED interactions. However, the motion of fission and fusion products induced by the nuclear interaction produces photons as these ions scatter off of each other by their electrostatic potentials. These photons are in the $100$KeV to $1$ MeV range of energy.
Neutrons are produced, and in the case of fusion they constitute $18$MeV of energy produced per fusion $D~+~T~\rightarrow~{}_2^4He~+~n$, which in turn produce photons as secondaries when they interact with matter. There is the neutron bomb that is a $T-T$ nuclear bomb meant to produce lots of neutrons. These have a magnetic moment that they interact with matter, and these are damaging to biological molecules. The neutron bomb is then largely an anti-personnel weapon and fashioned into a mini-hydrogen bomb.
As a comment in general, it will be interesting to see if our species finally gets out of the obsession over these before we end up using them in a global war.
