220:
22:
194:
While almost all accelerator lattices that are in use in modern facilities are specifically designed for their particular purpose, the lattice development starts at a given ideal lattice design with high periodicity and mostly using only one base cell. The most widely known are
156:. The lattice properties have a large influence on the properties of the particle beam, which is shaped by magnetic fields. Lattices can be closed (cyclic accelerators like the
43:
261:
94:
66:
285:
113:
73:
80:
254:
47:
62:
290:
167:
Such a structure is needed for focusing of the particle beam in modern, large-scale facilities. Its basic elements are
32:
205:
51:
36:
247:
164:
facilities) and are also used at interconnects between different accelerator structures (transfer beamlines).
87:
153:
184:
149:
127:
187:, and sometimes even higher order magnets. Many lattices are composed of identical substructures or
227:
137:
199:
191:, which denote a special magnet arrangement that may reoccur at several positions along the path.
172:
231:
180:
219:
176:
279:
168:
145:
157:
131:
21:
211:
A Magnet
Accelerator is very important for fast moving of objects.
161:
15:
148:
at given longitudinal positions around the vacuum tube of a
202:, which is the simplest possible strong focusing lattice
235:
255:
8:
50:. Unsourced material may be challenged and
262:
248:
152:, and thus along the path of the enclosed
114:Learn how and when to remove this message
7:
216:
214:
48:adding citations to reliable sources
63:"Magnetic lattice" accelerator
234:. You can help Knowledge (XXG) by
14:
218:
20:
1:
307:
213:
125:
286:Accelerator physics stubs
230:-related article is a
206:Chasman–Green lattice
154:charged particle beam
185:chromatic aberration
150:particle accelerator
144:is a composition of
128:Particle accelerator
44:improve this article
291:Accelerator physics
228:accelerator physics
138:accelerator physics
183:for correction of
173:quadrupole magnets
243:
242:
181:sextupole magnets
124:
123:
116:
98:
298:
264:
257:
250:
222:
215:
171:for deflection,
142:magnetic lattice
119:
112:
108:
105:
99:
97:
56:
24:
16:
306:
305:
301:
300:
299:
297:
296:
295:
276:
275:
274:
269:
268:
177:strong focusing
160:), linear (for
134:
120:
109:
103:
100:
57:
55:
41:
25:
12:
11:
5:
304:
302:
294:
293:
288:
278:
277:
273:
270:
267:
266:
259:
252:
244:
241:
240:
223:
209:
208:
203:
169:dipole magnets
146:electromagnets
122:
121:
28:
26:
19:
13:
10:
9:
6:
4:
3:
2:
303:
292:
289:
287:
284:
283:
281:
271:
265:
260:
258:
253:
251:
246:
245:
239:
237:
233:
229:
224:
221:
217:
212:
207:
204:
201:
198:
197:
196:
192:
190:
186:
182:
178:
174:
170:
165:
163:
159:
155:
151:
147:
143:
139:
133:
129:
118:
115:
107:
96:
93:
89:
86:
82:
79:
75:
72:
68:
65: –
64:
60:
59:Find sources:
53:
49:
45:
39:
38:
34:
29:This article
27:
23:
18:
17:
236:expanding it
225:
210:
200:FODO lattice
193:
188:
166:
158:synchrotrons
141:
135:
110:
104:January 2023
101:
91:
84:
77:
70:
58:
42:Please help
30:
132:synchrotron
280:Categories
272:References
126:See also:
74:newspapers
31:does not
88:scholar
52:removed
37:sources
90:
83:
76:
69:
61:
226:This
189:cells
162:linac
95:JSTOR
81:books
232:stub
175:for
140:, a
130:and
67:news
35:any
33:cite
136:In
46:by
282::
179:,
263:e
256:t
249:v
238:.
117:)
111:(
106:)
102:(
92:·
85:·
78:·
71:·
54:.
40:.
Text is available under the Creative Commons Attribution-ShareAlike License. Additional terms may apply.
