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Ferrimagnetism

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179: 3359:; this magnetization is reached when the external field is strong enough to make all the moments align in the same direction. When this point is reached, the magnetization cannot increase, as there are no more moments to align. When the external field is removed, the magnetization of the ferrimagnet does not disappear, but a nonzero magnetization remains. This effect is often used in applications of magnets. If an external field in the opposite direction is applied subsequently, the magnet will demagnetize further until it eventually reaches a magnetization of 3266: 40: 67: 4112: 1091: 206:. An example of this can be seen in the figure above. Here the atoms with a smaller magnetic moment point in the opposite direction of the larger moments. This arrangement is similar to that present in antiferromagnetic materials, but in ferrimagnetic materials the net moment is nonzero because the opposed moments differ in magnitude. 3182: 165:
Sb, French physicist Charles Guillaud discovered that the current theories on magnetism were not adequate to explain the behavior of the material, and made a model to explain the behavior. In 1948, Néel published a paper about a third type of cooperative magnetism, based on the assumptions in
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Unlike ferromagnetism, the magnetization curves of ferrimagnetism can take many different shapes depending on the strength of the interactions and the relative abundance of atoms. The most notable instances of this property are that the direction of magnetization can reverse while heating a
3253:, but at which the opposing magnetic moments are equal (resulting in a net magnetic moment of zero) is called a magnetization compensation point. This compensation point is observed easily in garnets and rare-earth–transition-metal alloys (RE-TM). Furthermore, ferrimagnets may also have an 2867: 3012: 2337: 2174: 3217:
to its critical temperature, and that strength of magnetization can increase while heating a ferrimagnetic material to the critical temperature, both of which cannot occur for ferromagnetic materials. These temperature dependencies have also been experimentally observed in
843: 48: 3441:; when it is polarized in the opposite direction, the interaction is very low. When the interaction is strong, the microwave signal can pass through the material. This directional property is used in the construction of microwave devices like 1673: 1541: 58: 57: 666: 3061: 1885: 2725: 2558: 2450: 2873: 1978: 2180: 2020: 182:➀ Below the magnetization compensation point, ferrimagnetic material is magnetic. ➁ At the compensation point, the magnetic components cancel each other, and the total magnetic moment is zero. ➂ Above the 1086:{\displaystyle {\vec {H}}_{aa}=\gamma _{aa}{\vec {M}},\quad {\vec {H}}_{ab}=\gamma _{ab}{\vec {M}}_{b},\quad {\vec {H}}_{ba}=\gamma _{ba}{\vec {M}}_{a},\quad {\vec {H}}_{bb}=\gamma _{bb}{\vec {M}}_{b}.} 310: 3646: 221:, and the system can no longer maintain a spontaneous magnetization. This is because at higher temperatures the thermal motion is strong enough that it exceeds the tendency of the dipoles to align. 1787: 1730: 446: 4080:
Sessoli, Roberta; Tsai, Hui Lien; Schake, Ann R.; Wang, Sheyi; Vincent, John B.; Folting, Kirsten; Gatteschi, Dante; Christou, George; Hendrickson, David N. (1993). "High-spin molecules: ".
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is actually induced by an external applied field. When this applied field aligns with the magnetic dipoles, it causes a net magnetic dipole moment and causes the magnetic dipoles to
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compensation point, at which the net angular momentum vanishes. This compensation point is crucial for achieving fast magnetization reversal in magnetic-memory devices.
526: 477: 2597: 795: 546: 497: 53: 2008: 3202: 3854: 775: 554: 3461:. Ferrimagnetic minerals in various rock types are used to study ancient geomagnetic properties of Earth and other planets. That field of study is known as 4040:"Natural Magnetite for thermal energy storage: Excellent thermophysical properties, reversible latent heat transition and controlled thermal conductivity" 198:. In ferrimagnetic materials the magnetization is also caused by a combination of dipole–dipole interactions and exchange interactions resulting from the 3177:{\displaystyle F(\lambda ,\alpha ,\beta )={\frac {1}{2}}\left(\lambda \alpha +\mu \beta +{\sqrt {(\lambda \alpha -\mu \beta )^{2}+4\lambda \mu }}\right)} 4144: 2862:{\displaystyle \lambda \sigma _{a}={\frac {\tau F(\lambda ,\alpha ,\beta )}{\alpha \beta -1}}(\beta \tanh ^{-1}\sigma _{a}+\tanh ^{-1}\sigma _{b}),} 1795: 3007:{\displaystyle \mu \sigma _{b}={\frac {\tau F(\lambda ,\alpha ,\beta )}{\alpha \beta -1}}(\tanh ^{-1}\sigma _{a}+\alpha \tanh ^{-1}\sigma _{b})} 2456: 2348: 52: 4016: 3995:
Soler, M. A. G.; Paterno, L. G. (2017-01-01), Da Róz, Alessandra L.; Ferreira, Marystela; de Lima Leite, Fábio; Oliveira, Osvaldo N. (eds.),
3877: 3830: 3621: 1891: 178: 2332:{\displaystyle {\vec {H}}_{b}={\vec {H}}_{0}+Ng\mu _{B}S_{b}\gamma _{ab}(-\lambda {\vec {\sigma }}_{a}+\mu \beta {\vec {\sigma }}_{b}).} 2169:{\displaystyle {\vec {H}}_{a}={\vec {H}}_{0}+Ng\mu _{B}S_{a}\gamma _{ab}(\lambda \alpha {\vec {\sigma }}_{a}-\mu {\vec {\sigma }}_{b}),} 3184:. These equations do not have a known analytical solution, so they must be solved numerically to find the temperature dependence of 161:
published a paper proposing the existence of a new form of cooperative magnetism he called antiferromagnetism. While working with Mn
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discovered ferrimagnetism in 1948. Since the discovery, numerous uses have been found for ferrimagnetic materials, such as
4137: 3571: = 10 derived from antiferromagnetic interaction on Mn(IV) metal centers with Mn(III) and Mn(II) metal centers. 218: 4232: 1735: 1681: 394: 3269: 1789:
which give the ratio between the strengths of the interactions. At last we will introduce the reduced magnetizations
1145: 4287: 4116: 199: 95: 4130: 1099: 202:. The main difference is that in ferrimagnetic materials there are different types of atoms in the material's 3332:, where magnetic behavior depends on the history of the magnet. They also exhibit a saturation magnetization 4292: 4189: 166:
Guillaud's model. He called it ferrimagnetism. In 1970, Néel was awarded for his work in magnetism with the
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Until the twentieth century, all naturally occurring magnetic substances were called ferromagnets. In 1936,
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as a positive quantity and write the minus sign explicitly in front of it. For the total fields on
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sites of its crystal structure exhibit opposite spin. Other known ferrimagnetic materials include
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Grosu, Yaroslav; Faik, Abdessamad; Ortega-Fernández, Iñigo; D'Aguanno, Bruno (March 2017).
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When ferrimagnets are exposed to an external magnetic field, they display what is called
3965: 3918: 3767: 3720: 3665: 3265: 661:{\displaystyle {\vec {H}}_{i}={\vec {H}}_{0}+\sum _{k=1}^{n}\gamma _{ik}{\vec {M}}_{k},} 391:
is field caused by the interactions between the atoms. The following assumption then is
4249: 4222: 4207: 4008: 3609: 3462: 3280: 760: 191: 39: 31: 3950:"Reversal of Spontaneous Magnetization as a Function of Temperature in LiFeCr Spinels" 4281: 4244: 4239: 4179: 3689: 3273: 3214: 210: 158: 138: 118: 110: 4167: 3647:"Propriétés magnétiques des ferrites ; ferrimagnétisme et antiferromagnétisme" 3290:. The downward curve after saturation, along with the lower return curve, form the 3751: 3728: 3673: 4056: 4039: 3704: 3402: 146: 749:-th substructures. For a diatomic lattice we can designate two types of sites, 229:
There are various ways to describe ferrimagnets, the simplest of which is with
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remains. This can for example occur when the populations consist of different
66: 3981: 3973: 3934: 3887: 3840: 3783: 3736: 3681: 3631: 17: 4153: 3564: 3514: 3482: 3466: 3430: 3320: 1880:{\displaystyle {\vec {\sigma }}_{a}={\vec {M}}_{a}/\lambda Ng\mu _{B}S_{a},} 548:
to be position- and orientation-dependent, we can then write it in the form
203: 126: 4111: 3902: 4264: 3926: 3502: 2553:{\displaystyle \sigma _{b}=B_{S_{b}}(g\mu _{b}S_{b}H_{b}/k_{\text{B}}T).} 2445:{\displaystyle \sigma _{a}=B_{S_{a}}(g\mu _{b}S_{a}H_{a}/k_{\text{B}}T),} 78:
compound, is one of the most common examples of a ferrimagnetic material.
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Klein, C. and Dutrow, B., Mineral Science, 23rd ed., Wiley, p. 243.
3521:; and hexagonal or spinel type ferrites, including rhenium ferrite, ReFe 3450: 1973:{\displaystyle {\vec {\sigma }}_{b}={\vec {M}}_{b}/\mu Ng\mu _{B}S_{b}} 233:. In mean-field theory the field acting on the atoms can be written as 75: 62:
Magnetic orders: comparison between ferro, antiferro and ferrimagnetism
3775: 3903:"Magnetic Properties of Ferrite-Chromite Series of Nickel and Cobalt" 3510: 3506: 3437:
in the same direction as this precession strongly interacts with the
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material is a material that has populations of atoms with opposing
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The solutions to these equations (omitted here) are then given by
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Ferrimagnets have a critical temperature above which they become
3518: 137:), is ferrimagnetic, but was classified as a ferromagnet before 99: 4126: 103: 4122: 3465:. In addition, it has been shown that ferrimagnets such as 305:{\displaystyle {\vec {H}}={\vec {H}}_{0}+{\vec {H}}_{m},} 213:
just as ferromagnets do. At this temperature (called the
3616:(2nd ed.). Cambridge: Cambridge University Press. 3614:
Magnetic materials : fundamentals and applications
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at a frequency controlled by the applied field, called
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substances, ferrimagnetic substances are attracted by
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favors an anti-parallel alignment. For ferrimagnets,
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Pages displaying wikidata descriptions as a fallback
4200: 4160: 3453:. Ferrimagnetic materials are also used to produce 2719:, this then gives the following pair of equations: 94:, but these moments are unequal in magnitude, so a 3868:Blundell, Stephen; Blundell, Katherine M. (2010). 3381: 3351: 3286:. Starting at the origin, the upward curve is the 3196: 3176: 3050: 3006: 2861: 2711: 2649: 2591: 2552: 2444: 2331: 2168: 2002: 1972: 1879: 1781: 1724: 1667: 1535: 1393: 1363: 1327: 1291: 1255: 1219: 1183: 1134: 1085: 825: 789: 769: 733: 699: 660: 540: 520: 499:is the molecular field coefficient. When we allow 491: 471: 440: 383: 343: 304: 3872:(2nd ed.). Oxford: Oxford University Press. 1782:{\displaystyle \beta =\gamma _{bb}/\gamma _{ab},} 1725:{\displaystyle \alpha =\gamma _{aa}/\gamma _{ab}} 479:is the average magnetization of the lattice, and 441:{\displaystyle {\vec {H}}_{m}=\gamma {\vec {M}}.} 190:Ferrimagnetism has the same physical origins as 4003:, William Andrew Publishing, pp. 147–186, 741:is the molecular field coefficient between the 1678:Furthermore, we will introduce the parameters 1184:{\displaystyle \gamma _{aa}\neq \gamma _{bb},} 4138: 3948:Gorter, E. W.; Schulkes, J. A. (1953-05-01). 2014:-th element. This then gives for the fields: 777:the number of magnetic ions per unit volume, 8: 3389:. This behavior results in what is called a 4145: 4131: 4123: 3853:: CS1 maint: location missing publisher ( 4055: 3373: 3364: 3343: 3337: 3189: 3149: 3125: 3092: 3063: 3042: 3033: 3022: 2995: 2979: 2963: 2947: 2893: 2884: 2875: 2847: 2831: 2818: 2802: 2745: 2736: 2727: 2672: 2668: 2662: 2639: 2627: 2614: 2608: 2574: 2568: 2535: 2526: 2520: 2510: 2500: 2482: 2477: 2464: 2458: 2427: 2418: 2412: 2402: 2392: 2374: 2369: 2356: 2350: 2317: 2306: 2305: 2289: 2278: 2277: 2258: 2248: 2238: 2219: 2208: 2207: 2197: 2186: 2185: 2182: 2154: 2143: 2142: 2129: 2118: 2117: 2098: 2088: 2078: 2059: 2048: 2047: 2037: 2026: 2025: 2022: 1994: 1988: 1964: 1954: 1936: 1930: 1919: 1918: 1908: 1897: 1896: 1893: 1868: 1858: 1840: 1834: 1823: 1822: 1812: 1801: 1800: 1797: 1767: 1758: 1749: 1737: 1713: 1704: 1695: 1683: 1656: 1645: 1644: 1634: 1621: 1610: 1609: 1599: 1586: 1575: 1574: 1564: 1553: 1552: 1549: 1524: 1513: 1512: 1502: 1489: 1478: 1477: 1467: 1454: 1443: 1442: 1432: 1421: 1420: 1417: 1382: 1376: 1346: 1340: 1310: 1304: 1283: 1272: 1271: 1268: 1247: 1236: 1235: 1232: 1202: 1196: 1169: 1153: 1147: 1135:{\displaystyle \gamma _{ab}=\gamma _{ba}} 1123: 1107: 1101: 1074: 1063: 1062: 1052: 1036: 1025: 1024: 1013: 1002: 1001: 991: 975: 964: 963: 952: 941: 940: 930: 914: 903: 902: 886: 885: 876: 860: 849: 848: 845: 806: 797:the fraction of the magnetic ions on the 782: 762: 722: 716: 691: 680: 679: 676: 649: 638: 637: 627: 617: 606: 593: 582: 581: 571: 560: 559: 556: 533: 507: 506: 504: 484: 458: 457: 455: 424: 423: 411: 400: 399: 396: 375: 364: 363: 360: 335: 324: 323: 320: 293: 282: 281: 271: 260: 259: 244: 243: 241: 3997:"Chapter 6. Magnetic Nanomaterials" 3907:Journal of the Physical Society of Japan 125:. The oldest known magnetic substance, 3601: 3563:. A classic example is a dodecanuclear 4044:Solar Energy Materials and Solar Cells 3846: 3583: – energy in a specific direction 1191:unless the structures are identical. 7: 3485:, is a ferrimagnetic substance. The 3481:The oldest known magnetic material, 3051:{\displaystyle \tau =T/T_{\text{c}}} 2603:. The simplest case to solve now is 3752:"The Néel Theory of Ferrimagnetism" 3750:Smart, J. Samuel (September 1955). 2712:{\displaystyle B_{1/2}(x)=\tanh(x)} 1371:, so it will be convenient to take 4009:10.1016/b978-0-323-49782-4.00006-1 3497:(YIG); cubic ferrites composed of 3401:Ferrimagnetic materials have high 25: 3901:Tsushima, Tachiro (August 1963). 3821:Simon, Steven H. (21 June 2013). 3798:"The Nobel Prize in Physics 1970" 3559:Ferrimagnetism can also occur in 1364:{\displaystyle \gamma _{ab}<0} 1328:{\displaystyle \gamma _{ab}<0} 1220:{\displaystyle \gamma _{ab}>0} 4110: 3567:molecule with an effective spin 2650:{\displaystyle S_{a}=S_{b}=1/2} 1227:favors a parallel alignment of 1022: 961: 900: 826:{\displaystyle \mu =1-\lambda } 186:, the material loses magnetism. 3382:{\displaystyle -M_{\text{rs}}} 3146: 3127: 3086: 3068: 3001: 2940: 2920: 2902: 2853: 2792: 2772: 2754: 2706: 2700: 2688: 2682: 2586: 2580: 2544: 2490: 2436: 2382: 2323: 2311: 2283: 2267: 2213: 2191: 2160: 2148: 2123: 2107: 2053: 2031: 1924: 1902: 1828: 1806: 1650: 1615: 1580: 1558: 1518: 1483: 1448: 1426: 1292:{\displaystyle {\vec {M}}_{b}} 1277: 1256:{\displaystyle {\vec {M}}_{a}} 1241: 1068: 1030: 1007: 969: 946: 908: 891: 854: 700:{\displaystyle {\vec {H}}_{i}} 685: 643: 587: 565: 512: 463: 429: 405: 384:{\displaystyle {\vec {H}}_{m}} 369: 344:{\displaystyle {\vec {H}}_{0}} 329: 287: 265: 249: 1: 3823:The Oxford Solid State Basics 3429:. As a particular example, a 3352:{\displaystyle M_{\text{rs}}} 3249:A temperature lower than the 219:second-order phase transition 4233:ferromagnetic superconductor 4057:10.1016/j.solmat.2016.12.006 3501:with other elements such as 3213:ferrimagnetic material from 1394:{\displaystyle \gamma _{ab}} 734:{\displaystyle \gamma _{ik}} 3870:Concepts in thermal physics 3756:American Journal of Physics 3729:10.1051/anphys/193611050232 3674:10.1051/anphys/194812030137 3288:initial magnetization curve 707:is the field acting on the 27:Type of magnetic phenomenon 4309: 521:{\displaystyle {\vec {M}}} 472:{\displaystyle {\vec {M}}} 29: 3261:Effect of external fields 200:Pauli exclusion principle 96:spontaneous magnetization 3974:10.1103/physrev.90.487.2 3825:(1st ed.). Oxford. 2592:{\displaystyle B_{J}(x)} 790:{\displaystyle \lambda } 30:Not to be confused with 4190:Van Vleck paramagnetism 3645:Néel, M. Louis (1948). 3561:single-molecule magnets 3439:magnetic dipole moments 837:sites. This then gives 541:{\displaystyle \gamma } 492:{\displaystyle \gamma } 3471:thermal energy storage 3383: 3353: 3325: 3208:Effects of temperature 3198: 3178: 3052: 3008: 2863: 2713: 2651: 2593: 2554: 2446: 2333: 2170: 2004: 1974: 1881: 1783: 1726: 1669: 1537: 1395: 1365: 1329: 1293: 1257: 1221: 1185: 1136: 1087: 827: 791: 771: 735: 711:-th substructure, and 701: 662: 622: 542: 522: 493: 473: 442: 385: 353:applied magnetic field 345: 306: 187: 168:Nobel Prize in Physics 79: 63: 44: 43:Ferrimagnetic ordering 3590:Orbital magnetization 3384: 3354: 3268: 3199: 3179: 3053: 3009: 2864: 2714: 2652: 2594: 2555: 2447: 2334: 2171: 2005: 2003:{\displaystyle S_{i}} 1975: 1882: 1784: 1727: 1670: 1538: 1396: 1366: 1330: 1294: 1258: 1222: 1186: 1137: 1096:It can be shown that 1088: 828: 792: 772: 736: 702: 663: 602: 543: 523: 494: 474: 443: 386: 346: 307: 181: 106:(such as Fe and Fe). 69: 61: 42: 4119:at Wikimedia Commons 3927:10.1143/jpsj.18.1162 3703:Néel, Louis (1936). 3435:circularly polarized 3426:precession frequency 3363: 3336: 3321:saturation remanence 3197:{\displaystyle \mu } 3188: 3062: 3021: 2874: 2726: 2661: 2607: 2567: 2457: 2349: 2181: 2021: 1987: 1892: 1796: 1736: 1682: 1548: 1416: 1375: 1339: 1303: 1267: 1231: 1195: 1146: 1100: 844: 833:the fraction on the 805: 781: 761: 715: 675: 555: 532: 503: 483: 454: 395: 359: 319: 240: 4260:amorphous magnetism 4228:superferromagnetism 4094:10.1021/ja00058a027 3966:1953PhRv...90..487G 3919:1963JPSJ...18.1162T 3768:1955AmJPh..23..356S 3721:1936AnPh...11..232N 3709:Annales de Physique 3666:1948AnPh...12..137N 3654:Annales de Physique 3495:yttrium iron garnet 3397:Properties and uses 3330:magnetic hysteresis 757:. We can designate 4213:antiferromagnetism 4185:superparamagnetism 3610:Spaldin, Nicola A. 3379: 3349: 3326: 3194: 3174: 3048: 3004: 2859: 2709: 2647: 2601:Brillouin function 2589: 2550: 2442: 2329: 2166: 2000: 1970: 1877: 1779: 1722: 1665: 1533: 1391: 1361: 1325: 1289: 1253: 1217: 1181: 1132: 1083: 823: 787: 767: 731: 697: 658: 538: 518: 489: 469: 438: 381: 341: 302: 196:antiferromagnetism 188: 92:antiferromagnetism 80: 70:Ferrite magnets. 64: 45: 4288:Magnetic ordering 4275: 4274: 4173:superdiamagnetism 4161:Magnetic response 4115:Media related to 4018:978-0-323-49782-4 3879:978-0-19-956209-1 3832:978-0-19-150210-1 3776:10.1119/1.1934006 3623:978-0-521-88669-7 3581:Anisotropy energy 3455:optical isolators 3376: 3346: 3294:. The intercepts 3270:Theoretical model 3251:Curie temperature 3167: 3100: 3045: 2938: 2790: 2538: 2430: 2314: 2286: 2216: 2194: 2151: 2126: 2056: 2034: 1927: 1905: 1831: 1809: 1653: 1618: 1583: 1561: 1521: 1486: 1451: 1429: 1280: 1244: 1071: 1033: 1010: 972: 949: 911: 894: 857: 770:{\displaystyle N} 688: 646: 590: 568: 515: 466: 432: 408: 372: 332: 290: 268: 252: 231:mean-field theory 215:Curie temperature 184:Curie temperature 123:permanent magnets 59: 16:(Redirected from 4300: 4147: 4140: 4133: 4124: 4114: 4098: 4097: 4088:(5): 1804–1816. 4082:J. Am. Chem. Soc 4077: 4071: 4068: 4062: 4061: 4059: 4035: 4029: 4027: 4026: 4025: 3992: 3986: 3985: 3945: 3939: 3938: 3913:(8): 1162–1166. 3898: 3892: 3891: 3865: 3859: 3858: 3852: 3844: 3818: 3812: 3811: 3809: 3808: 3794: 3788: 3787: 3747: 3741: 3740: 3700: 3694: 3693: 3651: 3642: 3636: 3635: 3606: 3586: 3469:can be used for 3409:properties. The 3388: 3386: 3385: 3380: 3378: 3377: 3374: 3358: 3356: 3355: 3350: 3348: 3347: 3344: 3311: 3302: 3285: 3278: 3255:angular momentum 3203: 3201: 3200: 3195: 3183: 3181: 3180: 3175: 3173: 3169: 3168: 3154: 3153: 3126: 3101: 3093: 3057: 3055: 3054: 3049: 3047: 3046: 3043: 3037: 3013: 3011: 3010: 3005: 3000: 2999: 2987: 2986: 2968: 2967: 2955: 2954: 2939: 2937: 2923: 2894: 2889: 2888: 2868: 2866: 2865: 2860: 2852: 2851: 2839: 2838: 2823: 2822: 2810: 2809: 2791: 2789: 2775: 2746: 2741: 2740: 2718: 2716: 2715: 2710: 2681: 2680: 2676: 2656: 2654: 2653: 2648: 2643: 2632: 2631: 2619: 2618: 2598: 2596: 2595: 2590: 2579: 2578: 2559: 2557: 2556: 2551: 2540: 2539: 2536: 2530: 2525: 2524: 2515: 2514: 2505: 2504: 2489: 2488: 2487: 2486: 2469: 2468: 2451: 2449: 2448: 2443: 2432: 2431: 2428: 2422: 2417: 2416: 2407: 2406: 2397: 2396: 2381: 2380: 2379: 2378: 2361: 2360: 2338: 2336: 2335: 2330: 2322: 2321: 2316: 2315: 2307: 2294: 2293: 2288: 2287: 2279: 2266: 2265: 2253: 2252: 2243: 2242: 2224: 2223: 2218: 2217: 2209: 2202: 2201: 2196: 2195: 2187: 2175: 2173: 2172: 2167: 2159: 2158: 2153: 2152: 2144: 2134: 2133: 2128: 2127: 2119: 2106: 2105: 2093: 2092: 2083: 2082: 2064: 2063: 2058: 2057: 2049: 2042: 2041: 2036: 2035: 2027: 2010:the spin of the 2009: 2007: 2006: 2001: 1999: 1998: 1979: 1977: 1976: 1971: 1969: 1968: 1959: 1958: 1940: 1935: 1934: 1929: 1928: 1920: 1913: 1912: 1907: 1906: 1898: 1886: 1884: 1883: 1878: 1873: 1872: 1863: 1862: 1844: 1839: 1838: 1833: 1832: 1824: 1817: 1816: 1811: 1810: 1802: 1788: 1786: 1785: 1780: 1775: 1774: 1762: 1757: 1756: 1731: 1729: 1728: 1723: 1721: 1720: 1708: 1703: 1702: 1674: 1672: 1671: 1666: 1661: 1660: 1655: 1654: 1646: 1642: 1641: 1626: 1625: 1620: 1619: 1611: 1607: 1606: 1591: 1590: 1585: 1584: 1576: 1569: 1568: 1563: 1562: 1554: 1542: 1540: 1539: 1534: 1529: 1528: 1523: 1522: 1514: 1510: 1509: 1494: 1493: 1488: 1487: 1479: 1475: 1474: 1459: 1458: 1453: 1452: 1444: 1437: 1436: 1431: 1430: 1422: 1409:this then gives 1400: 1398: 1397: 1392: 1390: 1389: 1370: 1368: 1367: 1362: 1354: 1353: 1334: 1332: 1331: 1326: 1318: 1317: 1298: 1296: 1295: 1290: 1288: 1287: 1282: 1281: 1273: 1262: 1260: 1259: 1254: 1252: 1251: 1246: 1245: 1237: 1226: 1224: 1223: 1218: 1210: 1209: 1190: 1188: 1187: 1182: 1177: 1176: 1161: 1160: 1141: 1139: 1138: 1133: 1131: 1130: 1115: 1114: 1092: 1090: 1089: 1084: 1079: 1078: 1073: 1072: 1064: 1060: 1059: 1044: 1043: 1035: 1034: 1026: 1018: 1017: 1012: 1011: 1003: 999: 998: 983: 982: 974: 973: 965: 957: 956: 951: 950: 942: 938: 937: 922: 921: 913: 912: 904: 896: 895: 887: 884: 883: 868: 867: 859: 858: 850: 832: 830: 829: 824: 796: 794: 793: 788: 776: 774: 773: 768: 740: 738: 737: 732: 730: 729: 706: 704: 703: 698: 696: 695: 690: 689: 681: 667: 665: 664: 659: 654: 653: 648: 647: 639: 635: 634: 621: 616: 598: 597: 592: 591: 583: 576: 575: 570: 569: 561: 547: 545: 544: 539: 527: 525: 524: 519: 517: 516: 508: 498: 496: 495: 490: 478: 476: 475: 470: 468: 467: 459: 447: 445: 444: 439: 434: 433: 425: 416: 415: 410: 409: 401: 390: 388: 387: 382: 380: 379: 374: 373: 365: 350: 348: 347: 342: 340: 339: 334: 333: 325: 311: 309: 308: 303: 298: 297: 292: 291: 283: 276: 275: 270: 269: 261: 254: 253: 245: 88:magnetic moments 60: 21: 4308: 4307: 4303: 4302: 4301: 4299: 4298: 4297: 4278: 4277: 4276: 4271: 4201:Magnetic states 4196: 4156: 4151: 4107: 4102: 4101: 4079: 4078: 4074: 4069: 4065: 4037: 4036: 4032: 4023: 4021: 4019: 3994: 3993: 3989: 3954:Physical Review 3947: 3946: 3942: 3900: 3899: 3895: 3880: 3867: 3866: 3862: 3845: 3833: 3820: 3819: 3815: 3806: 3804: 3796: 3795: 3791: 3749: 3748: 3744: 3702: 3701: 3697: 3649: 3644: 3643: 3639: 3624: 3608: 3607: 3603: 3598: 3584: 3577: 3555: 3544: 3540: 3536: 3532: 3528: 3524: 3479: 3399: 3391:hysteresis loop 3369: 3361: 3360: 3339: 3334: 3333: 3310: 3307: 3304: 3301: 3298: 3295: 3283: 3276: 3263: 3245: 3241: 3237: 3233: 3229: 3225: 3221: 3210: 3186: 3185: 3145: 3106: 3102: 3060: 3059: 3038: 3019: 3018: 2991: 2975: 2959: 2943: 2924: 2895: 2880: 2872: 2871: 2843: 2827: 2814: 2798: 2776: 2747: 2732: 2724: 2723: 2664: 2659: 2658: 2623: 2610: 2605: 2604: 2570: 2565: 2564: 2531: 2516: 2506: 2496: 2478: 2473: 2460: 2455: 2454: 2423: 2408: 2398: 2388: 2370: 2365: 2352: 2347: 2346: 2304: 2276: 2254: 2244: 2234: 2206: 2184: 2179: 2178: 2141: 2116: 2094: 2084: 2074: 2046: 2024: 2019: 2018: 1990: 1985: 1984: 1960: 1950: 1917: 1895: 1890: 1889: 1864: 1854: 1821: 1799: 1794: 1793: 1763: 1745: 1734: 1733: 1709: 1691: 1680: 1679: 1643: 1630: 1608: 1595: 1573: 1551: 1546: 1545: 1511: 1498: 1476: 1463: 1441: 1419: 1414: 1413: 1378: 1373: 1372: 1342: 1337: 1336: 1306: 1301: 1300: 1270: 1265: 1264: 1234: 1229: 1228: 1198: 1193: 1192: 1165: 1149: 1144: 1143: 1119: 1103: 1098: 1097: 1061: 1048: 1023: 1000: 987: 962: 939: 926: 901: 872: 847: 842: 841: 803: 802: 779: 778: 759: 758: 718: 713: 712: 678: 673: 672: 636: 623: 580: 558: 553: 552: 530: 529: 501: 500: 481: 480: 452: 451: 398: 393: 392: 362: 357: 356: 322: 317: 316: 280: 258: 238: 237: 227: 176: 174:Physical origin 164: 155: 136: 132: 47: 35: 28: 23: 22: 15: 12: 11: 5: 4306: 4304: 4296: 4295: 4293:Quantum phases 4290: 4280: 4279: 4273: 4272: 4270: 4269: 4268: 4267: 4262: 4252: 4250:mictomagnetism 4247: 4242: 4237: 4236: 4235: 4230: 4223:ferromagnetism 4220: 4218:ferrimagnetism 4215: 4210: 4208:altermagnetism 4204: 4202: 4198: 4197: 4195: 4194: 4193: 4192: 4187: 4177: 4176: 4175: 4164: 4162: 4158: 4157: 4152: 4150: 4149: 4142: 4135: 4127: 4121: 4120: 4117:Ferrimagnetism 4106: 4105:External links 4103: 4100: 4099: 4072: 4063: 4030: 4017: 4001:Nanostructures 3987: 3960:(3): 487–488. 3940: 3893: 3878: 3860: 3831: 3813: 3802:NobelPrize.org 3789: 3762:(6): 356–370. 3742: 3715:(5): 232–279. 3695: 3660:(3): 137–198. 3637: 3622: 3600: 3599: 3597: 3594: 3593: 3592: 3587: 3576: 3573: 3550: 3542: 3538: 3534: 3530: 3526: 3522: 3478: 3475: 3463:paleomagnetism 3398: 3395: 3372: 3368: 3342: 3308: 3305: 3299: 3296: 3281:magnetic field 3262: 3259: 3243: 3239: 3235: 3231: 3227: 3223: 3219: 3209: 3206: 3193: 3172: 3166: 3163: 3160: 3157: 3152: 3148: 3144: 3141: 3138: 3135: 3132: 3129: 3124: 3121: 3118: 3115: 3112: 3109: 3105: 3099: 3096: 3091: 3088: 3085: 3082: 3079: 3076: 3073: 3070: 3067: 3041: 3036: 3032: 3029: 3026: 3015: 3014: 3003: 2998: 2994: 2990: 2985: 2982: 2978: 2974: 2971: 2966: 2962: 2958: 2953: 2950: 2946: 2942: 2936: 2933: 2930: 2927: 2922: 2919: 2916: 2913: 2910: 2907: 2904: 2901: 2898: 2892: 2887: 2883: 2879: 2869: 2858: 2855: 2850: 2846: 2842: 2837: 2834: 2830: 2826: 2821: 2817: 2813: 2808: 2805: 2801: 2797: 2794: 2788: 2785: 2782: 2779: 2774: 2771: 2768: 2765: 2762: 2759: 2756: 2753: 2750: 2744: 2739: 2735: 2731: 2708: 2705: 2702: 2699: 2696: 2693: 2690: 2687: 2684: 2679: 2675: 2671: 2667: 2646: 2642: 2638: 2635: 2630: 2626: 2622: 2617: 2613: 2588: 2585: 2582: 2577: 2573: 2561: 2560: 2549: 2546: 2543: 2534: 2529: 2523: 2519: 2513: 2509: 2503: 2499: 2495: 2492: 2485: 2481: 2476: 2472: 2467: 2463: 2452: 2441: 2438: 2435: 2426: 2421: 2415: 2411: 2405: 2401: 2395: 2391: 2387: 2384: 2377: 2373: 2368: 2364: 2359: 2355: 2340: 2339: 2328: 2325: 2320: 2313: 2310: 2303: 2300: 2297: 2292: 2285: 2282: 2275: 2272: 2269: 2264: 2261: 2257: 2251: 2247: 2241: 2237: 2233: 2230: 2227: 2222: 2215: 2212: 2205: 2200: 2193: 2190: 2176: 2165: 2162: 2157: 2150: 2147: 2140: 2137: 2132: 2125: 2122: 2115: 2112: 2109: 2104: 2101: 2097: 2091: 2087: 2081: 2077: 2073: 2070: 2067: 2062: 2055: 2052: 2045: 2040: 2033: 2030: 1997: 1993: 1981: 1980: 1967: 1963: 1957: 1953: 1949: 1946: 1943: 1939: 1933: 1926: 1923: 1916: 1911: 1904: 1901: 1887: 1876: 1871: 1867: 1861: 1857: 1853: 1850: 1847: 1843: 1837: 1830: 1827: 1820: 1815: 1808: 1805: 1778: 1773: 1770: 1766: 1761: 1755: 1752: 1748: 1744: 1741: 1719: 1716: 1712: 1707: 1701: 1698: 1694: 1690: 1687: 1676: 1675: 1664: 1659: 1652: 1649: 1640: 1637: 1633: 1629: 1624: 1617: 1614: 1605: 1602: 1598: 1594: 1589: 1582: 1579: 1572: 1567: 1560: 1557: 1543: 1532: 1527: 1520: 1517: 1508: 1505: 1501: 1497: 1492: 1485: 1482: 1473: 1470: 1466: 1462: 1457: 1450: 1447: 1440: 1435: 1428: 1425: 1388: 1385: 1381: 1360: 1357: 1352: 1349: 1345: 1324: 1321: 1316: 1313: 1309: 1286: 1279: 1276: 1250: 1243: 1240: 1216: 1213: 1208: 1205: 1201: 1180: 1175: 1172: 1168: 1164: 1159: 1156: 1152: 1129: 1126: 1122: 1118: 1113: 1110: 1106: 1094: 1093: 1082: 1077: 1070: 1067: 1058: 1055: 1051: 1047: 1042: 1039: 1032: 1029: 1021: 1016: 1009: 1006: 997: 994: 990: 986: 981: 978: 971: 968: 960: 955: 948: 945: 936: 933: 929: 925: 920: 917: 910: 907: 899: 893: 890: 882: 879: 875: 871: 866: 863: 856: 853: 822: 819: 816: 813: 810: 786: 766: 728: 725: 721: 694: 687: 684: 669: 668: 657: 652: 645: 642: 633: 630: 626: 620: 615: 612: 609: 605: 601: 596: 589: 586: 579: 574: 567: 564: 537: 514: 511: 488: 465: 462: 437: 431: 428: 422: 419: 414: 407: 404: 378: 371: 368: 338: 331: 328: 313: 312: 301: 296: 289: 286: 279: 274: 267: 264: 257: 251: 248: 226: 223: 192:ferromagnetism 175: 172: 162: 154: 151: 149:applications. 134: 130: 32:Ferromagnetism 26: 24: 14: 13: 10: 9: 6: 4: 3: 2: 4305: 4294: 4291: 4289: 4286: 4285: 4283: 4266: 4263: 4261: 4258: 4257: 4256: 4253: 4251: 4248: 4246: 4245:metamagnetism 4243: 4241: 4240:helimagnetism 4238: 4234: 4231: 4229: 4226: 4225: 4224: 4221: 4219: 4216: 4214: 4211: 4209: 4206: 4205: 4203: 4199: 4191: 4188: 4186: 4183: 4182: 4181: 4180:paramagnetism 4178: 4174: 4171: 4170: 4169: 4166: 4165: 4163: 4159: 4155: 4148: 4143: 4141: 4136: 4134: 4129: 4128: 4125: 4118: 4113: 4109: 4108: 4104: 4095: 4091: 4087: 4083: 4076: 4073: 4067: 4064: 4058: 4053: 4049: 4045: 4041: 4034: 4031: 4020: 4014: 4010: 4006: 4002: 3998: 3991: 3988: 3983: 3979: 3975: 3971: 3967: 3963: 3959: 3955: 3951: 3944: 3941: 3936: 3932: 3928: 3924: 3920: 3916: 3912: 3908: 3904: 3897: 3894: 3889: 3885: 3881: 3875: 3871: 3864: 3861: 3856: 3850: 3842: 3838: 3834: 3828: 3824: 3817: 3814: 3803: 3799: 3793: 3790: 3785: 3781: 3777: 3773: 3769: 3765: 3761: 3757: 3753: 3746: 3743: 3738: 3734: 3730: 3726: 3722: 3718: 3714: 3710: 3706: 3699: 3696: 3691: 3687: 3683: 3679: 3675: 3671: 3667: 3663: 3659: 3655: 3648: 3641: 3638: 3633: 3629: 3625: 3619: 3615: 3611: 3605: 3602: 3595: 3591: 3588: 3582: 3579: 3578: 3574: 3572: 3570: 3566: 3562: 3557: 3554: 3548: 3520: 3516: 3512: 3508: 3504: 3500: 3496: 3492: 3488: 3484: 3476: 3474: 3472: 3468: 3464: 3460: 3456: 3452: 3448: 3444: 3440: 3436: 3432: 3428: 3427: 3422: 3421: 3416: 3412: 3408: 3404: 3396: 3394: 3392: 3370: 3366: 3340: 3331: 3323: 3322: 3317: 3316: 3293: 3289: 3282: 3275: 3274:magnetization 3271: 3267: 3260: 3258: 3256: 3252: 3247: 3216: 3215:absolute zero 3207: 3205: 3191: 3170: 3164: 3161: 3158: 3155: 3150: 3142: 3139: 3136: 3133: 3130: 3122: 3119: 3116: 3113: 3110: 3107: 3103: 3097: 3094: 3089: 3083: 3080: 3077: 3074: 3071: 3065: 3039: 3034: 3030: 3027: 3024: 2996: 2992: 2988: 2983: 2980: 2976: 2972: 2969: 2964: 2960: 2956: 2951: 2948: 2944: 2934: 2931: 2928: 2925: 2917: 2914: 2911: 2908: 2905: 2899: 2896: 2890: 2885: 2881: 2877: 2870: 2856: 2848: 2844: 2840: 2835: 2832: 2828: 2824: 2819: 2815: 2811: 2806: 2803: 2799: 2795: 2786: 2783: 2780: 2777: 2769: 2766: 2763: 2760: 2757: 2751: 2748: 2742: 2737: 2733: 2729: 2722: 2721: 2720: 2703: 2697: 2694: 2691: 2685: 2677: 2673: 2669: 2665: 2644: 2640: 2636: 2633: 2628: 2624: 2620: 2615: 2611: 2602: 2583: 2575: 2571: 2547: 2541: 2532: 2527: 2521: 2517: 2511: 2507: 2501: 2497: 2493: 2483: 2479: 2474: 2470: 2465: 2461: 2453: 2439: 2433: 2424: 2419: 2413: 2409: 2403: 2399: 2393: 2389: 2385: 2375: 2371: 2366: 2362: 2357: 2353: 2345: 2344: 2343: 2326: 2318: 2308: 2301: 2298: 2295: 2290: 2280: 2273: 2270: 2262: 2259: 2255: 2249: 2245: 2239: 2235: 2231: 2228: 2225: 2220: 2210: 2203: 2198: 2188: 2177: 2163: 2155: 2145: 2138: 2135: 2130: 2120: 2113: 2110: 2102: 2099: 2095: 2089: 2085: 2079: 2075: 2071: 2068: 2065: 2060: 2050: 2043: 2038: 2028: 2017: 2016: 2015: 2013: 1995: 1991: 1965: 1961: 1955: 1951: 1947: 1944: 1941: 1937: 1931: 1921: 1914: 1909: 1899: 1888: 1874: 1869: 1865: 1859: 1855: 1851: 1848: 1845: 1841: 1835: 1825: 1818: 1813: 1803: 1792: 1791: 1790: 1776: 1771: 1768: 1764: 1759: 1753: 1750: 1746: 1742: 1739: 1717: 1714: 1710: 1705: 1699: 1696: 1692: 1688: 1685: 1662: 1657: 1647: 1638: 1635: 1631: 1627: 1622: 1612: 1603: 1600: 1596: 1592: 1587: 1577: 1570: 1565: 1555: 1544: 1530: 1525: 1515: 1506: 1503: 1499: 1495: 1490: 1480: 1471: 1468: 1464: 1460: 1455: 1445: 1438: 1433: 1423: 1412: 1411: 1410: 1408: 1404: 1386: 1383: 1379: 1358: 1355: 1350: 1347: 1343: 1322: 1319: 1314: 1311: 1307: 1284: 1274: 1248: 1238: 1214: 1211: 1206: 1203: 1199: 1178: 1173: 1170: 1166: 1162: 1157: 1154: 1150: 1127: 1124: 1120: 1116: 1111: 1108: 1104: 1080: 1075: 1065: 1056: 1053: 1049: 1045: 1040: 1037: 1027: 1019: 1014: 1004: 995: 992: 988: 984: 979: 976: 966: 958: 953: 943: 934: 931: 927: 923: 918: 915: 905: 897: 888: 880: 877: 873: 869: 864: 861: 851: 840: 839: 838: 836: 820: 817: 814: 811: 808: 800: 784: 764: 756: 752: 748: 744: 726: 723: 719: 710: 692: 682: 655: 650: 640: 631: 628: 624: 618: 613: 610: 607: 603: 599: 594: 584: 577: 572: 562: 551: 550: 549: 535: 509: 486: 460: 448: 435: 426: 420: 417: 412: 402: 376: 366: 354: 336: 326: 299: 294: 284: 277: 272: 262: 255: 246: 236: 235: 234: 232: 224: 222: 220: 217:) there is a 216: 212: 207: 205: 201: 197: 193: 185: 180: 173: 171: 169: 160: 152: 150: 148: 145:platters and 144: 140: 128: 124: 120: 116: 112: 111:ferromagnetic 107: 105: 101: 97: 93: 89: 85: 84:ferrimagnetic 77: 73: 68: 41: 37: 33: 19: 18:Ferrimagnetic 4217: 4168:diamagnetism 4085: 4081: 4075: 4066: 4047: 4043: 4033: 4022:, retrieved 4000: 3990: 3957: 3953: 3943: 3910: 3906: 3896: 3869: 3863: 3822: 3816: 3805:. Retrieved 3801: 3792: 3759: 3755: 3745: 3712: 3708: 3698: 3657: 3653: 3640: 3613: 3604: 3568: 3558: 3552: 3480: 3424: 3418: 3400: 3390: 3327: 3319: 3313: 3291: 3287: 3248: 3211: 3016: 2562: 2341: 2011: 1982: 1677: 1406: 1402: 1095: 834: 798: 754: 750: 746: 742: 708: 670: 449: 314: 228: 211:paramagnetic 208: 189: 156: 108: 83: 81: 36: 4050:: 170–176. 3499:iron oxides 3487:tetrahedral 3459:circulators 3447:circulators 3407:anisotropic 3403:resistivity 801:sites, and 117:and can be 4282:Categories 4255:spin glass 4024:2021-01-25 3807:2021-01-26 3596:References 3547:pyrrhotite 3491:octahedral 3411:anisotropy 3315:coercivity 225:Derivation 159:Louis Néel 147:biomedical 143:hard-drive 139:Louis Néel 119:magnetized 4154:Magnetism 3982:0031-899X 3935:0031-9015 3888:607907330 3849:cite book 3841:851099021 3784:0002-9505 3737:0003-4169 3690:126111103 3682:0003-4169 3632:607986416 3565:manganese 3515:manganese 3483:magnetite 3467:magnetite 3443:isolators 3431:microwave 3405:and have 3367:− 3292:main loop 3192:μ 3165:μ 3162:λ 3143:β 3140:μ 3137:− 3134:α 3131:λ 3120:β 3117:μ 3111:α 3108:λ 3084:β 3078:α 3072:λ 3025:τ 2993:σ 2989:⁡ 2981:− 2973:α 2961:σ 2957:⁡ 2949:− 2932:− 2929:β 2926:α 2918:β 2912:α 2906:λ 2897:τ 2882:σ 2878:μ 2845:σ 2841:⁡ 2833:− 2816:σ 2812:⁡ 2804:− 2796:β 2784:− 2781:β 2778:α 2770:β 2764:α 2758:λ 2749:τ 2734:σ 2730:λ 2698:⁡ 2498:μ 2462:σ 2390:μ 2354:σ 2312:→ 2309:σ 2302:β 2299:μ 2284:→ 2281:σ 2274:λ 2271:− 2256:γ 2236:μ 2214:→ 2192:→ 2149:→ 2146:σ 2139:μ 2136:− 2124:→ 2121:σ 2114:α 2111:λ 2096:γ 2076:μ 2054:→ 2032:→ 1952:μ 1942:μ 1925:→ 1903:→ 1900:σ 1856:μ 1846:λ 1829:→ 1807:→ 1804:σ 1765:γ 1747:γ 1740:β 1711:γ 1693:γ 1686:α 1651:→ 1632:γ 1628:− 1616:→ 1597:γ 1581:→ 1559:→ 1519:→ 1500:γ 1496:− 1484:→ 1465:γ 1449:→ 1427:→ 1380:γ 1344:γ 1308:γ 1278:→ 1242:→ 1200:γ 1167:γ 1163:≠ 1151:γ 1142:and that 1121:γ 1105:γ 1069:→ 1050:γ 1031:→ 1008:→ 989:γ 970:→ 947:→ 928:γ 909:→ 892:→ 874:γ 855:→ 821:λ 818:− 809:μ 785:λ 720:γ 686:→ 644:→ 625:γ 604:∑ 588:→ 566:→ 536:γ 513:→ 487:γ 464:→ 430:→ 421:γ 406:→ 370:→ 330:→ 288:→ 266:→ 250:→ 204:unit cell 127:magnetite 4265:spin ice 3612:(2011). 3575:See also 3537:and BaFe 3503:aluminum 3477:Examples 3451:gyrators 3312:are the 3279:against 2657:. 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Index

Ferrimagnetic
Ferromagnetism


Ferrite
ceramic
magnetic moments
antiferromagnetism
spontaneous magnetization
atoms
ions
ferromagnetic
magnets
magnetized
permanent magnets
magnetite
Louis Néel
hard-drive
biomedical
Louis Néel
Nobel Prize in Physics

Curie temperature
ferromagnetism
antiferromagnetism
Pauli exclusion principle
unit cell
paramagnetic
Curie temperature
second-order phase transition

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