Knowledge (XXG)

Sextupole magnet

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17: 41: 200:) is dependent on the energy of the particle being focused—high energy particles having longer focal lengths than those with lower energy. Since all realistic beams have some, non-negligible, energy spread, any focusing scheme that relies purely on quadrupole magnets will result in the size of the beam "blowing up" with distance. 248:
In addition, the quadrature dependence of the sextupole kick on the transverse offset of the beam, can lead to high amplitude particles being kicked far from the beam axis and being lost on the beam-pipe walls. Due to this mechanism, the addition of sextupole fields to an accelerator lattice will
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Sextupolar fields have a focal length that is inversely proportional to the distance from the center of the magnet with which the particle passes. This is similar to the action of a quadrupole, whose effect on the beam may be described as a bending whose strength depends on the distance from the
180: 233:), then the sextupole can be set at a strength that ensures that particles of all reasonable energy offsets are focused to the same point. This will negate the tendency of the quadrupole lattice to disperse the beam. 241:
Sextupolar fields are non-linear (i.e. they depend on the product of the sizes of the transverse displacements), and have terms which depend on both the horizontal and vertical offsets (i.e. they are coupled).
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This leads to equations of motion that cannot be solved for the general case, thus requiring approximations to be used when calculating their effects on the beam.
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that flows in the coils of wire wrapped around the poles. The coils may be formed from hollow copper magnet wire that carry coolant, usually de-ionized water. The
127: 250: 56:) consist of six magnetic poles set out in an arrangement of alternating north and south poles arranged around an axis. They are used in 229:
If a sextupole is placed at a point at which the particles in the beam are arranged by their energy offset (i.e. a region of non-zero
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used to focus and combine the beam have the unfortunate property that their focusing strength (describable by a
40: 65: 25: 266: 57: 114: 77: 61: 29: 230: 204: 314: 117:, magnetic deflection is more powerful than electrostatic, and use of the magnetic term of the 291: 193: 99:
of such a conductor can be above 10 amps/mm (four times that of standard copper conductors).
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Field lines of an idealized sextupole magnet in the plane transverse to the beam direction
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is enabled with various magnets that make up 'the lattice' required to bend, steer and
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Typically this is controlled with the addition of sextupolar fields to the lattice.
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of the ring (the tendency for off-energy particles to have different values for the
212: 208: 197: 21: 175:{\displaystyle \mathbf {F} =q(\mathbf {E} +\mathbf {v} \times \mathbf {B} ),} 216: 33: 207:
this is due to the under- or over-focusing of the particles, while in
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pole tips of alternating polarity. The steel is magnetised by a large
69: 88: 39: 15: 130: 174: 317:. The European X-Ray Laser Project (XFEL). n.d 8: 20:Sextupole electromagnet as used within the 161: 153: 145: 131: 129: 303: 113:At the energies reached in high energy 309: 307: 7: 14: 74:transmission electron microscopes 162: 154: 146: 132: 83:The design of sextupoles using 166: 142: 1: 363: 219:phase advance per orbit). 106: 189:a charged particle beam. 103:In particle accelerators 68:. Two sets of sextupole 87:generally involves six 226:center of the magnet. 176: 45: 37: 26:Australian Synchrotron 267:Charged particle beam 211:it is related to the 177: 115:particle accelerators 66:head tail instability 62:chromatic aberrations 58:particle accelerators 43: 30:chromatic aberrations 19: 257:of the accelerator. 128: 78:spherical aberration 64:and for damping the 342:Accelerator physics 205:linear accelerators 60:for the control of 315:"Sextupole magnet" 194:quadrupole magnets 172: 46: 38: 292:Quadrupole magnet 52:(also known as a 354: 347:Types of magnets 326: 325: 323: 322: 311: 287:Multipole magnet 282:Halbach cylinder 251:dynamic aperture 181: 179: 178: 173: 165: 157: 149: 135: 93:electric current 50:sextupole magnet 362: 361: 357: 356: 355: 353: 352: 351: 332: 331: 330: 329: 320: 318: 313: 312: 305: 300: 277:Electron optics 263: 239: 126: 125: 111: 109:Strong focusing 105: 97:current density 76:to correct for 54:hexapole magnet 12: 11: 5: 360: 358: 350: 349: 344: 334: 333: 328: 327: 302: 301: 299: 296: 295: 294: 289: 284: 279: 274: 269: 262: 259: 238: 235: 183: 182: 171: 168: 164: 160: 156: 152: 148: 144: 141: 138: 134: 107:Main article: 104: 101: 85:electromagnets 13: 10: 9: 6: 4: 3: 2: 359: 348: 345: 343: 340: 339: 337: 316: 310: 308: 304: 297: 293: 290: 288: 285: 283: 280: 278: 275: 273: 272:Dipole magnet 270: 268: 265: 264: 260: 258: 256: 252: 246: 243: 236: 234: 232: 227: 223: 220: 218: 214: 210: 209:storage rings 206: 201: 199: 195: 190: 188: 169: 158: 150: 139: 136: 124: 123: 122: 120: 119:Lorentz force 116: 110: 102: 100: 98: 94: 90: 86: 81: 79: 75: 71: 67: 63: 59: 55: 51: 42: 35: 31: 27: 23: 18: 319:. Retrieved 247: 244: 240: 228: 224: 221: 213:chromaticity 202: 198:focal length 191: 184: 112: 82: 72:are used in 53: 49: 47: 22:storage ring 28:to correct 336:Categories 321:2008-09-17 298:References 255:acceptance 249:limit the 231:dispersion 159:× 261:See also 237:Problems 217:betatron 34:electron 70:magnets 32:of the 24:of the 187:focus 89:steel 192:The 36:beam 253:or 203:In 338:: 306:^ 121:: 80:. 48:A 324:. 170:, 167:) 163:B 155:v 151:+ 147:E 143:( 140:q 137:= 133:F

Index


storage ring
Australian Synchrotron
chromatic aberrations
electron

particle accelerators
chromatic aberrations
head tail instability
magnets
transmission electron microscopes
spherical aberration
electromagnets
steel
electric current
current density
Strong focusing
particle accelerators
Lorentz force
focus
quadrupole magnets
focal length
linear accelerators
storage rings
chromaticity
betatron
dispersion
dynamic aperture
acceptance
Charged particle beam

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