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The remainder of the chapter introduces the reader to the theory of diatomic molecules in laser fields.
The first two of these exist as diatomic gases at room temperature, and the latter two form diatomic vapors at moderately elevated temperatures.
High harmonic generation in atomic and diatomic molecular gases using intense picosecond laser pulses-a comparison.
This gives a relatively simple three-species gas mixture, of the type used in experimental facilities, which allows dissociation and recombination of the diatomic species.
This result is similar to that for a diatomic molecular ion.
This suggests that the fragment ions are ejected in opposite directions and the molecule behaves as a diatomic in the intense laser field.
Of course, electron and ion collisions with diatomic molecules have not been considered, which would accelerate dissociation.
However, no consideration is made for diatomic molecules.
The molecule hence seems to behave as a diatomic, with the fragment ions being ejected along the field direction.
To give it its technical description, it is a blue gaseous allotrope of oxygen derived or formed naturally from diatomic oxygen by electric discharge or exposure to ultra-violet radiation.
In this reaction a hydrogen atom is removed from the alkane, then replaced by a halogen atom by reaction with a diatomic halogen molecule.
The newly formed diatomic molecules initially have a very high vibrational temperature that efficiently transforms the vibrational energy into radiant energy; i.e., radiative heat flux.
Oxygen is the only one of the simple diatomic molecules (and one of the few molecules in general) to carry a magnetic moment.
For a diatomic molecule, the geometry is defined by the length of a single bond.
In the vapour phase it is a diatomic molecule.