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Tricritical point

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529: 82:) (thus, each point in this region corresponds to a triple point). This region will terminate in two critical lines of two-phase coexistence; these two critical lines may then terminate at a single tricritical point. This point is therefore "twice critical", since it belongs to two critical branches. 104:
It seems more convenient experimentally to consider mixtures with four components for which one thermodynamic variable (usually the pressure or the volume) is kept fixed. The situation then reduces to the one described for mixtures of three components.
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in 1937, wherein Landau called the tricritical point as the critical point of the continuous transition. The first example of the tricritical point was shown by
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number of components for which these points can appear. In this case, one may have a two-dimensional region of three-phase coexistence (
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Griffiths, R. B. (1970). Thermodynamics near the two-fluid critical mixing point in He 3-He 4. Physical Review Letters, 24(13), 715.
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undergoes a first- or a second-order phase transition. The question was finally settled in 1982. If the Ginzburg–Landau parameter
570: 70:). For tricritical points to be observed, one needs a mixture with more components. It can be shown that three is the 96:
turn out to apply for real systems in three dimensions (but not for systems whose spatial dimension is 2 or lower).
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A. S. Freitas & Douglas F. de Albuquerque (2015). "Existence of a tricritical point in the antiferromagnet KFe
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where type-I goes over into type-II superconductor. The prediction was confirmed in 2002 by Monte Carlo
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Landau, L. D., & Lifshitz, E. M. (2013). Statistical Physics: Volume 5 (Vol. 5). Elsevier.
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Landau, L. D. (1937). On the theory of phase transitions. I. Zh. Eksp. Teor. Fiz., 11, 19.
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curve meets the first order phase transition curve, which was first introduced by
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terminates. This definition is clearly parallel to the definition of an ordinary
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is different from that of a conventional critical point: the upper
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as the point at which two-phase coexistence terminates.
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Historically, it was for a long time unclear whether a
192: 154: 118: 466: 216: 178: 124: 581: 54:A point of three-phase coexistence is termed a 564: 148:order. The tricritical point lies at roughly 403: 358: 571: 557: 487: 427: 19:refers to a point where the second order 179:{\displaystyle \kappa =0.76/{\sqrt {2}}} 58:for a one-component system, since, from 582: 217:{\displaystyle \kappa =1/{\sqrt {2}}} 523: 13: 92:is lowered from d=4 to d=3 so the 14: 611: 467:J. Hove; S. Mo; A. Sudbo (2002). 31:in helium-3 helium-4 mixture. In 527: 460: 397: 352: 293: 281: 264: 255: 246: 237: 99: 1: 231: 543:. You can help Knowledge by 7: 272:Theory of Phase Equilibrium 186:, slightly below the value 10: 616: 522: 506:10.1103/PhysRevB.66.064524 338:10.1103/PhysRevE.91.012117 140:superconductors (see also 446:10.1209/epl/i2006-10029-5 537:condensed matter physics 371:Lettere al Nuovo Cimento 33:condensed matter physics 125:{\displaystyle \kappa } 45:three-phase coexistence 600:Condensed matter stubs 539:-related article is a 218: 180: 126: 219: 181: 127: 43:of a system at which 226:computer simulations 190: 152: 116: 498:2002PhRvB..66f4524H 438:2006EL.....74..889K 330:2015PhRvE..91a2117F 132:that distinguishes 94:classical exponents 29:Robert B. Griffiths 595:Critical phenomena 383:10.1007/BF02754760 278:, 100, 13190-13199 214: 176: 122: 90:critical dimension 39:is a point in the 590:Phase transitions 552: 551: 274:, J. Phys. Chem. 212: 174: 86:critical behavior 60:Gibbs' phase rule 37:tricritical point 17:Tricritical point 607: 573: 566: 559: 531: 524: 518: 517: 491: 489:cond-mat/0202215 473: 464: 458: 457: 431: 429:cond-mat/0509430 413: 401: 395: 394: 368: 356: 350: 349: 297: 291: 285: 279: 268: 262: 259: 253: 250: 244: 241: 223: 221: 220: 215: 213: 208: 206: 185: 183: 182: 177: 175: 170: 168: 131: 129: 128: 123: 21:phase transition 615: 614: 610: 609: 608: 606: 605: 604: 580: 579: 578: 577: 521: 471: 465: 461: 411: 402: 398: 377:(13): 405–412. 366: 357: 353: 311: 307: 303: 298: 294: 286: 282: 269: 265: 260: 256: 251: 247: 242: 238: 234: 207: 202: 191: 188: 187: 169: 164: 153: 150: 149: 117: 114: 113: 102: 83: 12: 11: 5: 613: 603: 602: 597: 592: 576: 575: 568: 561: 553: 550: 549: 532: 520: 519: 459: 422:(5): 889–895. 416:Europhys. Lett 396: 351: 314:kagome lattice 309: 305: 301: 292: 280: 263: 254: 245: 235: 233: 230: 211: 205: 201: 198: 195: 173: 167: 163: 160: 157: 121: 110:superconductor 101: 98: 49:critical point 9: 6: 4: 3: 2: 612: 601: 598: 596: 593: 591: 588: 587: 585: 574: 569: 567: 562: 560: 555: 554: 548: 546: 542: 538: 533: 530: 526: 525: 515: 511: 507: 503: 499: 495: 490: 485: 482:(6): 064524. 481: 477: 470: 463: 455: 451: 447: 443: 439: 435: 430: 425: 421: 417: 410: 406: 400: 392: 388: 384: 380: 376: 372: 365: 361: 355: 347: 343: 339: 335: 331: 327: 324:(1): 012117. 323: 319: 315: 296: 289: 284: 277: 273: 267: 258: 249: 240: 236: 229: 227: 209: 203: 199: 196: 193: 171: 165: 161: 158: 155: 147: 143: 139: 135: 119: 111: 106: 97: 95: 91: 87: 81: 77: 73: 69: 65: 61: 57: 52: 50: 46: 42: 41:phase diagram 38: 34: 30: 26: 22: 18: 545:expanding it 534: 479: 475: 462: 419: 415: 399: 374: 370: 354: 321: 318:Phys. Rev. E 317: 295: 287: 283: 275: 271: 266: 257: 248: 239: 145: 107: 103: 84:Indeed, its 79: 75: 71: 67: 63: 56:triple point 53: 36: 16: 15: 405:H. Kleinert 360:H. Kleinert 100:Solid state 584:Categories 270:B. Widom, 232:References 25:Lev Landau 476:Phys. Rev 391:121012850 194:κ 156:κ 120:κ 78:= 2-3+3 = 66:= 2-3+1 = 514:13672575 454:55633766 407:(2006). 362:(1982). 346:25679580 494:Bibcode 434:Bibcode 326:Bibcode 138:type-II 72:minimum 512:  452:  389:  344:  146:second 134:type-I 535:This 510:S2CID 484:arXiv 472:(PDF) 450:S2CID 424:arXiv 412:(PDF) 387:S2CID 367:(PDF) 312:on a 308:(SO4) 541:stub 480:B 66 342:PMID 304:(OH) 288:ibid 276:1996 162:0.76 142:here 136:and 502:doi 442:doi 379:doi 334:doi 316:". 586:: 508:. 500:. 492:. 478:. 474:. 448:. 440:. 432:. 420:74 418:. 414:. 385:. 375:35 373:. 369:. 340:. 332:. 322:91 320:. 228:. 572:e 565:t 558:v 547:. 516:. 504:: 496:: 486:: 456:. 444:: 436:: 426:: 393:. 381:: 348:. 336:: 328:: 310:2 306:6 302:3 290:. 210:2 204:/ 200:1 197:= 172:2 166:/ 159:= 80:2 76:F 68:0 64:F

Index

phase transition
Lev Landau
Robert B. Griffiths
condensed matter physics
phase diagram
three-phase coexistence
critical point
triple point
Gibbs' phase rule
critical behavior
critical dimension
classical exponents
superconductor
type-I
type-II
here
computer simulations
kagome lattice
Bibcode
2015PhRvE..91a2117F
doi
10.1103/PhysRevE.91.012117
PMID
25679580
H. Kleinert
"Disorder Version of the Abelian Higgs Model and the Order of the Superconductive Phase Transition"
doi
10.1007/BF02754760
S2CID
121012850

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