Top view of the main apparatus Atomic hydrogen and deuterium are produced in two triple differentially pumped beam lines. The beams enter the main chamber (pressure in 10-10 torr range), where there is a sample holder and a quadrupole mass spectrometer to detect species coming off the sample. The top line can be converted into a He beam line, producing a He supersonic beam (about 1-2% velocity resolution) | |
| Side view | |
Deuterium Beam The beams are chopped by a mechanical selector to yield short pulses. At the top, D2 signal with radiofrequency turned off; at the bottom, undissociated deuterium (RF ON). | |
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Hydrogen beam source The source consists of a Pyrex tube, water-cooled, placed in a radiofrequency cavity consisting of a coil and a cylindrical shield. RF is fed into the cavity and hydrogen gets dissociated with efficiency of 75 to 90 %.The beam then goes through a collimator - which can be cooled to 150 K - and then into the first vacuum chamber of the beam line. Intensities of 1017 atoms/unit solid angle/sec are typically obtained. | |
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Low temperature sample holder The low temperature sample holder consist of a block of OFHC (oxygen free high conductivity) copper. There is a small cavity behind the plate holding the sample: a constantan filament, supported by a ceramic bowl, works as a heater for the sample. Two thermocouples and a silicon diode are used to monitor the temperature of the sample. Measurements are typically carried out in the temperature range of 5-30 K. There is also a sample manipulator (not shown) for studies in the 150-1000 K sample temperature range. |
![]() | Overview |
![]() | Beam Lines |
I. Atomic/Molecular Beam Scattering
Apparatus