Thermal beams: effusive sources

Atoms and thermostable molecules can be launched by heating in a resistively heated ceramic cell. Temperatures may range from about 500 K for vitamins to 900 K for intense fullerene beams.

For an ideal gas we would expect a Maxwell-Boltzmann distribution whose most probable velocity is determined by the energy balance kBT=mvmp2/2. For molecules in the mass range of 500-1000 amu and temperatures in ranging between 500-1000 K this corresponds to de Broglie wavelengths around ╬╗dB=3-6 pm. This is about 200-400 times smaller than the molecular diameter and about 1 Million times smaller than the transverse coherence that we prepare by passing the molecules through suitable apertures, further downstream.

Real sources have interactions between the molecules and are usually slighly faster than expected for purely effusive sources.  The source orifice measures typically 1 x 0.2 mm to be compatible with the geometry of our near-field interferometers.

Effusive sources are capable of ejecting thermally stable molecules at moderate forward velocity but high internal temperature, which we always assume to be equilibrated with the source temperature.

In the past, effusive sources have served in almost all KDTL interferometer experiments. We were able to use this method even for surprisingly massive particles, such as perfluoroalkyl-functionalized tetraphenylporphyrins. This molecules, synthesized in the group of Marcel Mayor in Basel, is designed to have low intermolecular binding and a low polarizability-to-mass-ratio.