A betatron is a type of cyclic particle accelerator for electrons. It consists of a torus-shaped vacuum chamber with an electron source. Circling the torus is an iron transformer core with a wire winding around it. The device functions similarly to a transformer, with the electrons in the torus-shaped vacuum chamber as its secondary coil. An alternating current in the primary coils accelerates electrons in the vacuum around a circular path. The betatron was the first machine capable of producing electron beams at energies higher than could be achieved with a simple electron gun, and the first circular accelerator in which particles orbited at a constant radius.
The concept of the betatron had been proposed as early as 1922 by Joseph Slepian. Through the 1920s and 30s a number of theoretical problems related to the device were considered by scientists including Rolf Wideroe, Ernest Walton, and Max Steenbeck. The first working betatron was constructed by Donald Kerst at the University of Illinois Urbana-Champaign in 1940.
After the discovery in the 1800s of Faraday's law of induction, which showed that an electromotive force could be generated by a changing magnetic field, several scientists speculated that this effect could be used to accelerate charged particles to high energies. Joseph Slepian proposed a device in 1922 that would use permanent magnets to steer the beam while it was accelerated by a changing magnetic field. However, he did not pursue the idea past the theoretical stage.
In the late 1920s, Gregory Breit and Merle Tuve at the Bureau of Terrestrial Magnetism constructed a working device that used varying magnetic fields to accelerate electrons. Their device placed two solenoidal magnets next to one another and fired electrons from a gun at the outer edge of the magnetic field. As the field was increased, the electrons accelerated in to strike a target at the center of the field, producing X-rays. This device took a step towards the betatron concept by shaping the magnetic field to keep the particles focused in the plane of acceleration.
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Un accélérateur de particules est un instrument qui utilise des champs électriques ou magnétiques pour amener des particules chargées électriquement à des vitesses élevées. En d'autres termes, il communique de l'énergie aux particules. On en distingue deux grandes catégories : les accélérateurs linéaires et les accélérateurs circulaires. En 2004, il y avait plus de dans le monde. Une centaine seulement sont de très grosses installations, nationales ou supranationales.
Un synchrotron est un instrument électromagnétique de grande taille destiné à l'accélération à haute énergie de particules élémentaires. Le plus grand accélérateur de type synchrotron est le Grand collisionneur de hadrons (LHC) de 27 kilomètres de circonférence, proche de Genève en Suisse, construit en 2008 par l'Organisation européenne pour la recherche nucléaire (CERN). Le principe du synchrotron a été presenté pendant la seconde guerre mondiale, en 1943, par le Oliphant à Birmingham.
thumb|upright=1.8|Diagramme animé montrant le fonctionnement d'un accélérateur linéaire thumb|Partie d'un accélérateur linéaire situé à Clayton, Victoria, Australie. Un accélérateur linéaire est un dispositif permettant d'accélérer des particules chargées afin de leur fournir une énergie cinétique importante dans le but de produire des réactions avec la matière. Les particules accélérées peuvent être des électrons, des protons, ou bien des ions lourds.
The grazing function g is introduced—a synchrobetatron optical quantity that is analogous (and closely connected) to the Twiss and dispersion functions β, α, η, and η′. It parametrizes the rate of change of total angle with respect to synchrotron amplitude ...
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American Vacuum Society2007
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