remsstrahlung (German pronunciation: ˈbʁɛmsˌʃtʁaːlʊŋ ( listen), from bremsen "to brake" and Strahlung "radiation", i.e. "braking radiation" or "deceleration radiation") is electromagnetic radiation produced by the deceleration of a answerable atom if deflected by addition answerable particle, about an electron by an diminutive nucleus. The affective atom loses active energy, which is adapted into a photon because activity is conserved. The appellation is aswell acclimated to accredit to the action of bearing the radiation. Bremsstrahlung has a connected spectrum, which becomes added acute and accouterment against college frequencies if the activity of the accelerated particles is increased.
Strictly speaking, bremsstrahlung refers to any radiation due to the dispatch of a answerable particle, which includes synchrotron radiation; however, it is frequently acclimated in the added attenuated faculty of radiation from electrons endlessly in matter.
Bremsstrahlung emitted from claret is sometimes referred to as free-free radiation. This refers to the actuality that the radiation in this case is created by answerable particles that are chargeless both afore and afterwards the angle (acceleration) that causes the emission.
Strictly speaking, bremsstrahlung refers to any radiation due to the dispatch of a answerable particle, which includes synchrotron radiation; however, it is frequently acclimated in the added attenuated faculty of radiation from electrons endlessly in matter.
Bremsstrahlung emitted from claret is sometimes referred to as free-free radiation. This refers to the actuality that the radiation in this case is created by answerable particles that are chargeless both afore and afterwards the angle (acceleration) that causes the emission.
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