生化分子質譜與光譜學實驗室
Laboratory for Mass Spectrometric and Spectroscopic Studies of Biomolecules

Molecular beam technique

What is a molecular beam?

        Molecular beams are high-density gas molecules flowing in the same direction at almost the same speed, so molecular beams have the following characteristics: (1) high flow rate of gas molecules, (2) all molecules move at the same speed, (3) all molecules go to the same direction, so there are no collisions between the molecules.

How are molecular beams generated?
        Pack gas molecules in a high-pressure (a few atmospheres) container, and force the gas molecules into the vacuum chamber through a small hole (about 100-500 microns in diameter). This is the process of isentropic expansion, also known as supersonic expansion. The flow of molecules about one mm in diameter in the middle is selected by means of a conical metal element (skimmer), which is the molecular beam. The main component of the pulsed molecular beam source is a pulsed gas valve; when the valve is closed, the high-pressure chamber and the vacuum chamber are isolated from each other; when the valve is opened, the gas is rushed into the vacuum chamber from the high-pressure chamber through the nozzle. If the pressure of the high-pressure chamber is high enough and the hole at the exit is small enough, the condition of free expansion can be achieved and a supersonic molecular beam can be generated. There are many types of pulse valves that generate pulsed molecular beams. The pulse valve we use (General Valve Corp, Series 9) is made using the mechanical principle of solenoid conductance. This pulse valve is operated by a pulse valve controller (a electric power supply which controls the frequency and trigger time of the pulse valve). In typical experiments, the trigger opening time is set to 100 microseconds, and the frequency is 10 Hz. Because the unit molecular density of the pulse type is higher than that of the continuous type, and the molecular velocity distribution is narrower, it is easy to assemble and has low background noise. The required pumping pump does not need a high pumping speed. It is more economical. The outlet nozzle diameter of the pulse valve we use is 0.15 mm in diameter, the top angle is 30 degrees, and 10.5 mm before the nozzle (nozzle). The skimmer is a conical stainless steel piece with a height of 20 mm, a top diameter of 1 mm, and a bottom diameter of 20 mm. The middle part of the generated supersonic molecular beam pass through the skimmer is usually referred to as molecular beam.

How can molecular beam technology be used?

       In the study of photodissociation or chemical reaction dynamics, this technique can be used to generate a single molecular collision event, with little background interference and greatly improved detection sensitivity. In molecular spectroscopy research, since molecular beams are generated through the process of adiabatic expansion, the probability of molecular rotation and vibration is reduced to a very low level, that is to say, molecules can be prepared in a ground state that hardly rotates or vibrates. So, the resolution of the molecular spectrum can be greatly improved, which is beneficial to distinguish complex chemical molecules. Molecular beam technology can also be used to prepare atomic or molecular clusters. Because of their special physical and chemical properties. This technology provides a new field of research for substances and materials. For example, clusters of cobalt atoms can be used as catalysts for oil cracking, clusters of silver atoms play a very important role in the imaging process of photographic negatives, clusters of carbon 60 may be the nanomaterials of the future, and the formation of acid rain in the atmosphere is also related to water and other molecules. Clusters are related. In terms of industrial applications, molecular beam technology can also be used to evaporate thin films, which is very relevant to the manufacture of semiconductor products.

References:
1. “Molecular Beams”, Norman F. Ramsey, Oxford University Press, New York, 1956.
2. “Molecular Beams and Low Density Gasdynamics”, Peter P. Wegener (ed.), Marcel Dekker, Inc., New York, 1974.
3. “Atomic and Molecular Beam Methods”, Giacinto Scoles (ed.), Oxford University Press, New York, 1988.


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