초록 ▼

A method for extracting a charged particle beam out of an isochronous cyclotron (1) comprising an electromagnet forming a magnetic circuit that includes at least a number of sectors (3, 3') known as "hills" where the air-gap is reduced, and separated by sector-shaped spaces (4) known as "valleys" wh

A method for extracting a charged particle beam out of an isochronous cyclotron (1) comprising an electromagnet forming a magnetic circuit that includes at least a number of sectors (3, 3') known as "hills" where the air-gap is reduced, and separated by sector-shaped spaces (4) known as "valleys" where the air-gap is larger. According to the extraction method, the particle beam is extracted without using an extraction device as the magnetic field has a special arrangement produced by designing the electromagnet air-gap at the "hills" (3, 3') of the isochronous cyclotron in such a way that the aspect ratio between the electromagnet air-gap at the "hills" in the region of the maximum radius, and the radius gain per turn of the particles accelerated by the cyclotron at said radius is less than 20.

대표청구항 ▼

[ I claim:] [1.] Method of extracting a beam of charged particles from an isochronous cyclotron (1) having an electromagnet constituting the magnetic circuit which includes at least a certain number of sectors (3, 3'), referred to as "hills", where the air gap is reduced, these being separated by sp

[ I claim:] [1.] Method of extracting a beam of charged particles from an isochronous cyclotron (1) having an electromagnet constituting the magnetic circuit which includes at least a certain number of sectors (3, 3'), referred to as "hills", where the air gap is reduced, these being separated by spaces in the form of sectors (4), referred to as "valleys", where the air gap is of larger size, the extraction method being characterized in that the particle beam is extracted by a particular arrangement of the magnetic field, without resorting to an extraction device, this arrangement being obtained by designing the air gap of the magnet at the hills (3, 3') of the isochronous cyclotron in such a way that the ratio of the dimension of the air gap of the magnet at the hills in the vicinity of-the maximum radius to the gain in radius per circuit of the particles accelerated by the cyclotron at this radius is less than 20.