Method and apparatus for storing an energy-rich electron beam in a race-track microtron

Claim 2

A race-track microtron for storing an energy-rich electron beam, and including a linear accelerator (1) arranged between two pairs of bending magnets (6, 7) such that said linear accelerator accelerates electrons and injects same into a magnetic field of one of said pairs of bending magnets, whereby said electrons travel in successive racetrack-like orbits of increasing width, in which each successive orbit has a common portion passing through said linear accelerator thereby repeatedly accelerating the electrons; a deflection magnet (9') and a septum magnet (9"), which are arranged in connection with the orbit (8) having the greatest diameter and a kicker magnet (16), characterized by a storage ring (10), closed on itself, for accelerated electrons arranged outside the septum magnet (9") and in the pole gap of each bending magnet (6, 7), said kicker magnet (16) being disposed in said storage ring (10) and in that two opposing pole surfaces in each bending magnet (6, 7) diverge outwardly, relative to the orbit (8) having the greatest diameter.

Claim 3

Race-track microtron as claimed in claim 1, wherein the electrons in the storage ring (10) have an energy of at least about 400 MeV, characterized in that the magnetic field in the area of the orbit (8) with the greatest diameter is in the order of magnitude of 1.75 T and that it diminishes successively to become about 1.4 T in the area of the storage ring (10), and in that the distance between said orbit and ring (9, 10) is about 2 dm.

Claim 4

Race-track microtron as claimed in claim 2, characterized in that a WIGGLER magnet (13) is placed in the storage ring for generating synchrotron light, and in that a cavity (15) is placed in the storage ring (10) for compensating the energy loss of the stored beam as a result of emitted synchrotron light.

Claim 5

Race-track microtron as claimed in claim 3, characterized in that the WIGGLER magnet has a strength of 6 T, whereby the critical wavelength for synchrotron light will be about 17 Å and in that the magnetic field of the bending magnets is 1.75 T, whereby the bending radius for the orbits in the race-track will be about 0.8 m.

Claim 6

Method of storing an energy-rich electron beam in a race-track microtron, which includes a linear accelerator (1) arranged between two pairs of bending magnets (6, 7) in which said linear accelerator accelerates electrons and injects same into a magnetic field of one of said pairs of bending magnets, whereby said electrons travel in successive racetrack-like orbits of increasing width, in which each successive orbit has a common portion passing through said linear accelerator thereby repeatedly accelerating the electrons; a deflection magnet (9') and a septum magnet (9") arranged in connection with the orbit (8) having the greatest diameter; and a kicker magnet for disturbing the state of equilibrium of an electron orbit, the method characterized by the steps of arranging the kicker magnet in a storage ring (10) situated outside the orbit (8) with the largest diameter and activating the kicker magnet for temporarily displacing an equilibrium orbit of the electrons in the storage ring (10) into the vicinity of a septum (17) of the septum magnet (9), injecting the electrons in the orbit (8) with the largest diameter into the temporarily displaced storage ring (20) by activating the septum magnet and subsequently successively deactivating the kicker magnet (16) whereby the equilibrium orbit for the storage ring moves outwards and contracts, inter alia as a result of the magnetic field between the pole surface of the two pairs of bending magnet diminishing in an outward direction relative to the orbit (8) with the greatest diameter.

Claim 7

Method of storing an energy-rich electron beam in a race-track microtron, which includes a linear accelerator (1) arranged between two pairs of bending magnets (6, 7) in which said linear accelerator accelerates electrons and injects same into a magnetic field of one of said pairs of bending magnets, whereby said electrons travel in successive racetrack-like orbits of increasing width, in which each successive orbit has a common portion passing through said linear accelerator thereby repeatedly accelerating the electrons; a deflection magnet (9') and a septum magnet (9") arranged in connection with the orbit (8) having the greatest diameter; and a kicker magnet for disturbing the state of equilibrium of an electron orbit, the method characterized by the steps of arranging the kicker magnet in a storage ring (10) situated outside the orbit (8) with the largest diameter and activating the kicker magnet for temporarily displacing an equilibrium orbit of the electrons in the storage ring (10) into the vicinity of a septum (17) of the septum magnet (9), injecting the electrons in the orbit (8) with the largest diameter into the temporarily displaced storage ring (20) by activating the septum magnet and subsequently successively deactivating the kicker magnet (16) whereby the equilibrium orbit for the storage ring moves outwards and contracts, inter alia as a result of the magnetic field between the pole surface of the two pairs of bending magnet diminishing in an outward direction relative to the orbit (8) with the greatest diameter.