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Non-perturbative

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solution is one that cannot be described in terms of perturbations about some simple background, such as empty space. For this reason, non-perturbative solutions and theories yield insights into areas and subjects that perturbative methods cannot reveal.
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In physics, such functions arise for phenomena which are impossible to understand by perturbation theory, at any finite order. In
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Schwinger, Julian (1951-06-01). "On Gauge Invariance and Vacuum Polarization".
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which cannot be expanded in a Taylor series in the electric charge
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are examples. A concrete, physical example is given by the
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is the mass of an electron and we have used units where
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Functions that can't be described by perturbation theory
131:= 0. Every coefficient of the Taylor expansion around 340: 320: 300: 280: 175: 135:= 0 is exactly zero, but the function is non-zero if 63: 358: 326: 306: 286: 263: 112: 627: 485:(5). American Physical Society (APS): 664–679. 50:or process is one that cannot be described by 610: 553: 31:is identically zero, but the function is not. 617: 603: 560: 546: 476: 470: 18: 454:Advanced Topics in Quantum Field Theory 448: 628: 442: 569: 512: 13: 224: 176: 113:{\displaystyle f(x)=e^{-1/x^{2}},} 14: 657: 347: 294:, or the electric field strength 573: 516: 456:. Cambridge University Press. 429:Causal dynamical triangulation 195: 185: 73: 67: 1: 435: 123:which does not equal its own 54:. An example is the function 589:. You can help Knowledge by 532:. You can help Knowledge by 7: 381: 148:'t Hooft–Polyakov monopoles 127:in any neighborhood around 10: 662: 568: 511: 414:Operator product expansion 359:{\displaystyle c=\hbar =1} 585:-related article is a 528:-related article is a 491:10.1103/physrev.82.664 360: 328: 308: 288: 265: 114: 32: 646:Quantum physics stubs 361: 329: 309: 289: 266: 115: 22: 424:Loop quantum gravity 338: 318: 298: 278: 173: 144:quantum field theory 61: 636:Perturbation theory 419:Conformal bootstrap 371:theoretical physics 52:perturbation theory 356: 324: 304: 284: 261: 110: 33: 641:Mathematics stubs 598: 597: 583:quantum mechanics 541: 540: 463:978-0-521-19084-8 327:{\displaystyle m} 307:{\displaystyle E} 287:{\displaystyle e} 257: 220: 653: 619: 612: 605: 577: 570: 562: 555: 548: 520: 513: 503: 502: 474: 468: 467: 446: 375:non-perturbative 365: 363: 362: 357: 333: 331: 330: 325: 313: 311: 310: 305: 293: 291: 290: 285: 270: 268: 267: 262: 260: 259: 258: 256: 248: 247: 246: 233: 227: 221: 219: 218: 217: 204: 203: 202: 183: 164:Schwinger effect 119: 117: 116: 111: 106: 105: 104: 103: 94: 45:non-perturbative 29:MacLaurin series 661: 660: 656: 655: 654: 652: 651: 650: 626: 625: 624: 623: 567: 566: 509: 507: 506: 479:Physical Review 475: 471: 464: 447: 443: 438: 433: 384: 339: 336: 335: 319: 316: 315: 299: 296: 295: 279: 276: 275: 249: 242: 238: 234: 232: 228: 223: 222: 213: 209: 205: 198: 194: 184: 182: 174: 171: 170: 99: 95: 90: 83: 79: 62: 59: 58: 17: 12: 11: 5: 659: 649: 648: 643: 638: 622: 621: 614: 607: 599: 596: 595: 578: 565: 564: 557: 550: 542: 539: 538: 521: 505: 504: 469: 462: 440: 439: 437: 434: 432: 431: 426: 421: 416: 411: 409:BCFW recursion 406: 401: 396: 391: 385: 383: 380: 355: 352: 349: 346: 343: 323: 303: 283: 272: 271: 255: 252: 245: 241: 237: 231: 226: 216: 212: 208: 201: 197: 193: 190: 187: 181: 178: 121: 120: 109: 102: 98: 93: 89: 86: 82: 78: 75: 72: 69: 66: 15: 9: 6: 4: 3: 2: 658: 647: 644: 642: 639: 637: 634: 633: 631: 620: 615: 613: 608: 606: 601: 600: 594: 592: 588: 584: 579: 576: 572: 571: 563: 558: 556: 551: 549: 544: 543: 537: 535: 531: 527: 522: 519: 515: 514: 510: 500: 496: 492: 488: 484: 480: 473: 465: 459: 455: 451: 445: 441: 430: 427: 425: 422: 420: 417: 415: 412: 410: 407: 405: 402: 400: 397: 395: 392: 390: 387: 386: 379: 376: 372: 367: 353: 350: 344: 341: 321: 301: 281: 253: 250: 243: 239: 235: 229: 214: 210: 206: 199: 191: 188: 179: 169: 168: 167: 165: 161: 157: 153: 149: 145: 140: 138: 134: 130: 126: 125:Taylor series 107: 100: 96: 91: 87: 84: 80: 76: 70: 64: 57: 56: 55: 53: 49: 46: 42: 38: 30: 26: 23:The function 21: 591:expanding it 580: 534:expanding it 523: 508: 482: 478: 472: 453: 444: 374: 368: 273: 152:domain walls 141: 136: 132: 128: 122: 44: 34: 24: 526:mathematics 450:Shifman, M. 389:Lattice QCD 37:mathematics 630:Categories 436:References 160:instantons 156:flux tubes 499:0031-899X 404:Instanton 399:Sphaleron 348:ℏ 236:π 230:− 211:π 177:Γ 85:− 452:(2012). 382:See also 48:function 394:Soliton 314:. Here 41:physics 497:  460:  158:, and 27:. The 581:This 524:This 139:≠ 0. 587:stub 530:stub 495:ISSN 458:ISBN 373:, a 43:, a 39:and 487:doi 369:In 35:In 632:: 493:. 483:82 481:. 366:. 154:, 150:, 146:, 618:e 611:t 604:v 593:. 561:e 554:t 547:v 536:. 501:. 489:: 466:. 354:1 351:= 345:= 342:c 322:m 302:E 282:e 254:E 251:e 244:2 240:m 225:e 215:3 207:4 200:2 196:) 192:E 189:e 186:( 180:= 137:x 133:x 129:x 108:, 101:2 97:x 92:/ 88:1 81:e 77:= 74:) 71:x 68:( 65:f 25:e

Index


MacLaurin series
mathematics
physics
function
perturbation theory
Taylor series
quantum field theory
't Hooft–Polyakov monopoles
domain walls
flux tubes
instantons
Schwinger effect
theoretical physics
Lattice QCD
Soliton
Sphaleron
Instanton
BCFW recursion
Operator product expansion
Conformal bootstrap
Loop quantum gravity
Causal dynamical triangulation
Shifman, M.
ISBN
978-0-521-19084-8
doi
10.1103/physrev.82.664
ISSN
0031-899X

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