Abstract
A theory for the intensities and shapes of fundamental band R1(J) and P1(J) lines of HD under pressures of rare gases is presented, with specific application to the R1(1) line of HD-Kr. The absorption contours principally consist of a broad (∼100 cm1) feature representing the ordinary intracollisional dipole intensity, and narrow components arising from the small HD permanent dipole moment function; permanent-dipole-collisionally-induced-dipole interference; and positive intercollisional interference between dipoles induced in successive collisions.
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