The Stark deceleration technique can produce molecular beams with very low velocities. In order to maximize the density of decelerated molecules, experimental parameters such as the velocity, the velocity spread and the spatial spread of the initial molecular beam as well as the operation characteristics of the decelerator have to be chosen appropriately. In this tutorial review, we describe procedures for the optimization of the density of Stark decelerated radicals for low-velocity applications which are of interest in, e.g., molecule trapping and cold-collision studies.
Keywords: Cold molecules, Molecular beams, Stark deceleration, Radicals
ReviewTranslationally cold molecules have become an attractive subject of research in recent years. A number of techniques for the generation of cold molecules has been developed [1-5] among which Stark deceleration is one of the most important [3,[6][7][8]. This method finds a broad range of applications in spectroscopy [9][10][11][12], collision-dynamics studies [13][14][15][16][17][18][19][20][21][22][23][24][25][26] and trap loading experiments [27][28][29][30][31][32][33]. The principle of Stark deceleration has been well documented [2,3], and a number of operation schemes have been developed for the optimization of Stark-decelerated molecular beams in different types of experiments [34][35][36][37].A Stark decelerator employs time-varying inhomogeneous electric fields produced by an array of dipolar electrodes to slow down pulsed beams of polar molecules [3,6]. When a packet of molecules approaches a set of electrodes, they are switched to high electric potential. Molecules in low-field-seeking Stark states experience a force which reduces their kinetic energy. The voltages on the electrodes are switched off before the molecules reach the maximum of the dipole potential in order to prevent their re-acceleration after they have passed the electrodes. This procedure is repeated at every pair of electrodes along the decelerator until the molecules have reached their target velocity at the exit of the assembly.The final velocity of the packet of molecules is controlled by a parameter referred to as phase angle 0 which corresponds to a scaled position of a "synchronous molecule" at which the high voltages on the electrodes of the decelerator are switched. Successful