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Froissart–Stora equation

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The original Froissart–Stora equation was derived for polarized protons. It may also be applied to polarized electrons in storage rings. In this case, there are additional polarization effects resulting from the synchrotron radiation. In particular, the
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The resonance may be crossed by raising the energy so that the spin tune passes through a resonance, or driven with a transverse magnetic field at a frequency that is in resonance with the spin oscillations.
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describes the polarization due to spin flip radiation. In the case of a non-planar ring, this must be generalized as was done by Derbenev and Kondratenko.
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Froissart, Marcel; Stora, Raymond (June 1960). "Depolarisation d'un faisceau de protons polarises dans un synchrotron".
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The Froissart–Stora equation has a direct analogy in condensed matter physics in the
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Turrin, A. (1982-02-08). "Dynamics of traversing an avoided level crossing".
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is the initial polarization before resonance crossing.
228: 201: 181: 53: 244: 214: 187: 164: 222:is the speed at which the resonance is crossed. 383: 36:tune. It is named after the French physicists 24:which a high energy charged particle beam in a 291: 266: 374:http://pra.aps.org/abstract/PRA/v37/i2/p456_1 327:http://iopscience.iop.org/0034-4885/68/9/R01/ 384: 338: 28:will undergo as it passes through a 13: 14: 413: 165:{\displaystyle P_{y}=P_{y0}\left} 294:Nuclear Instruments and Methods 397:Eponymous equations of physics 367: 332: 320: 285: 195:is the resonance strength and 118: 109: 1: 361:10.1016/0375-9601(82)90757-5 314:10.1016/0029-554X(60)90033-1 7: 267:Other spin-dynamics effects 215:{\displaystyle \alpha _{0}} 10: 418: 188:{\displaystyle \epsilon } 279: 20:describes the change in 18:Froissart–Stora equation 246: 245:{\displaystyle P_{y0}} 216: 189: 166: 274:Sokolov–Ternov effect 247: 217: 190: 167: 226: 199: 179: 51: 392:Accelerator physics 353:1982PhLA...87..455T 306:1960NucIM...7..297F 242: 212: 185: 162: 402:Quantum mechanics 341:Physics Letters A 144: 409: 377: 371: 365: 364: 336: 330: 324: 318: 317: 289: 251: 249: 248: 243: 241: 240: 221: 219: 218: 213: 211: 210: 194: 192: 191: 186: 171: 169: 168: 163: 161: 157: 150: 146: 145: 143: 142: 141: 128: 127: 126: 121: 112: 103: 79: 78: 63: 62: 38:Marcel Froissart 417: 416: 412: 411: 410: 408: 407: 406: 382: 381: 380: 372: 368: 337: 333: 325: 321: 290: 286: 282: 269: 233: 229: 227: 224: 223: 206: 202: 200: 197: 196: 180: 177: 176: 137: 133: 129: 122: 117: 116: 108: 104: 102: 98: 94: 84: 80: 71: 67: 58: 54: 52: 49: 48: 12: 11: 5: 415: 405: 404: 399: 394: 379: 378: 366: 347:(9): 455–456. 331: 319: 300:(3): 297–305. 283: 281: 278: 268: 265: 239: 236: 232: 209: 205: 184: 173: 172: 160: 156: 153: 149: 140: 136: 132: 125: 120: 115: 111: 107: 101: 97: 93: 90: 87: 83: 77: 74: 70: 66: 61: 57: 9: 6: 4: 3: 2: 414: 403: 400: 398: 395: 393: 390: 389: 387: 375: 370: 362: 358: 354: 350: 346: 342: 335: 328: 323: 315: 311: 307: 303: 299: 295: 288: 284: 277: 275: 264: 262: 257: 253: 237: 234: 230: 207: 203: 182: 158: 154: 151: 147: 138: 134: 130: 123: 113: 105: 99: 95: 91: 88: 85: 81: 75: 72: 68: 64: 59: 55: 47: 46: 45: 43: 42:Raymond Stora 39: 35: 31: 27: 23: 19: 369: 344: 340: 334: 322: 297: 293: 287: 270: 261:Landau–Zener 258: 254: 174: 26:storage ring 22:polarization 17: 15: 386:Categories 204:α 183:ϵ 152:− 135:α 114:ϵ 106:π 100:− 92:⁡ 30:resonance 263:effect. 349:Bibcode 302:Bibcode 32:in the 175:where 280:Notes 40:and 34:spin 16:The 357:doi 310:doi 89:exp 388:: 355:. 345:87 343:. 308:. 296:. 363:. 359:: 351:: 316:. 312:: 304:: 298:7 238:0 235:y 231:P 208:0 159:] 155:1 148:) 139:0 131:2 124:2 119:| 110:| 96:( 86:2 82:[ 76:0 73:y 69:P 65:= 60:y 56:P

Index

polarization
storage ring
resonance
spin
Marcel Froissart
Raymond Stora
Landau–Zener
Sokolov–Ternov effect
Bibcode
1960NucIM...7..297F
doi
10.1016/0029-554X(60)90033-1
http://iopscience.iop.org/0034-4885/68/9/R01/
Bibcode
1982PhLA...87..455T
doi
10.1016/0375-9601(82)90757-5
http://pra.aps.org/abstract/PRA/v37/i2/p456_1
Categories
Accelerator physics
Eponymous equations of physics
Quantum mechanics

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