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Molecular beam
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A molecular beam is produced by allowing a at higher to expand through a small orifice into a chamber at lower pressure to form a (, , or ) moving at approximately equal , with very few between the particles. Molecular beams are useful for fabricating in molecular beam epitaxy and artificial structures such as , , and . Molecular beams have also been applied as crossed molecular beams. The molecules in the molecular beam can be manipulated by and . Molecules can be decelerated in a Stark decelerator or in a .


History
The first to study atomic beam experiments was Louis Dunoyer de Segonzac 1911, but were simple experiments to confirm that atoms travelled in straight lines when not acted on by external forces.

In 1921, and wrote" about the deflection of beams of polar molecules in an inhomogeneous electric field, with an ultimate aim of measuring their dipole moments. Seeing the page proofs for the Kallman and Reiche work prompted at the University of Hamburg and University of Frankfurt am Main to rush publication of his work with on what later became known as the Stern–Gerlach experiment. (Stern's paper references the preprint, but the Kallman and Reiche work would go largely unnoticed.)

When the 1922 Stern-Gerlach paper appeared is caused a sensation: they claimed to have experimentally demonstrated "space quantization": clear evidence of quantum effects at a time when classical models were still considered viable. The initial quantum explanation of the measurement -- as an observation of orbital angular momentum -- was not correct. Five years of intense work on quantum theory was needed before it was realized that the experiment was in fact the first demonstration quantum electron spin Stern's group would go on to create pioneering experiments with atomic beams, and later with molecular beams. The advances of Stern and collaborators led to decisive discoveries including: the discovery of space quantization; de Broglie ; anomalous magnetic moments of the and ; of emission of a ; and the limitation of scattering cross-sections for molecular collisions imposed by the uncertainty principle

The first to report on the relationship between dipole moments and deflection in a molecular beam (using binary salts such as ) was Erwin Wrede in 1927."

In 1939 invented a molecular beam magnetic resonance method in which two magnets placed one after the other create an inhomogeneous magnetic field. The method was used to measure the of several lithium isotopes with molecular beams of , and . The Rabi molecular-beam method - The Feynman Lectures on Physics This method is a predecessor of . The invention of the in 1957 by James P. Gordon, Herbert J. Zeiger and Charles H. Townes was made possible by a molecular beam of and a special electrostatic quadrupole focuser.

The study of molecular beam led to the development of molecular-beam epitaxy in the 1960s.


See also
  • Norman Ramsey
  • John B. Fenn
  • F.M. Devienne
  • Dudley R. Herschbach

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