3087:
2645:
3082:{\displaystyle V=C+i\theta \chi -i{\overline {\theta }}{\overline {\chi }}+{\tfrac {i}{2}}\theta ^{2}(M+iN)-{\tfrac {i}{2}}{\overline {\theta ^{2}}}(M-iN)-\theta \sigma ^{\mu }{\overline {\theta }}A_{\mu }+i\theta ^{2}{\overline {\theta }}\left({\overline {\lambda }}+{\tfrac {i}{2}}{\overline {\sigma }}^{\mu }\partial _{\mu }\chi \right)-i{\overline {\theta }}^{2}\theta \left(\lambda +{\tfrac {i}{2}}\sigma ^{\mu }\partial _{\mu }{\overline {\chi }}\right)+{\tfrac {1}{2}}\theta ^{2}{\overline {\theta }}^{2}\left(D+{\tfrac {1}{2}}\Box C\right).}
772:
2298:
401:
2006:
3504:
767:{\displaystyle \Phi (x,\theta ,{\bar {\theta }})=\phi (x)+\theta \chi (x)+{\bar {\theta }}{\bar {\chi }}'(x)+{\bar {\theta }}\sigma ^{\mu }\theta V_{\mu }(x)+\theta ^{2}F(x)+{\bar {\theta }}^{2}{\bar {F}}'(x)+{\bar {\theta }}^{2}\theta \xi (x)+\theta ^{2}{\bar {\theta }}{\bar {\xi }}'(x)+\theta ^{2}{\bar {\theta }}^{2}D(x)}
2293:{\displaystyle \Phi (x,\theta ,{\bar {\theta }})=\phi (x)+{\sqrt {2}}\theta \psi (x)+\theta ^{2}F(x)+i\theta \sigma ^{\mu }{\bar {\theta }}\partial _{\mu }\phi (x)-{\frac {i}{\sqrt {2}}}\theta ^{2}\partial _{\mu }\psi (x)\sigma ^{\mu }{\bar {\theta }}-{\frac {1}{4}}\theta ^{2}{\bar {\theta }}^{2}\square \phi (x).}
1465:
2498:
3331:
893:
3612:
A scalar is never the highest component of a superfield; whether it appears in a superfield at all depends on the dimension of the spacetime. For example, in a 10-dimensional N=1 theory the vector multiplet contains only a vector and a
1624:
1339:
3625:
there is only one supermultiplet with a finite number of fields, the gravity multiplet, and it contains no scalars. However again its dimensional reduction on a d-torus to a maximal gravity multiplet does contain scalars.
1698:
1105:
2391:
3499:{\displaystyle V_{\text{WZ}}=\theta \sigma ^{\mu }{\bar {\theta }}A_{\mu }+\theta ^{2}{\bar {\theta }}{\bar {\lambda }}+{\bar {\theta }}^{2}\theta \lambda +{\frac {1}{2}}\theta ^{2}{\bar {\theta }}^{2}D.}
1842:
1518:
1266:
351:
3803:
2604:
1978:
1152:
1302:
4200:
2383:
1201:
947:
393:
286:
217:
175:
4238:
3221:
4350:
4312:
4275:
4155:
4125:
3982:
3944:
3886:
3832:
3670:
2551:
2344:
1756:
1727:
1049:
980:
3194:
4067:
3914:
3856:
2637:
1331:
61:
which is valued in such a representation. NaĂŻvely, or when considering flat superspace, a superfield can simply be viewed as a function on superspace. Formally, it is a
4784:
4038:
3558:
3527:
3254:
1783:
1011:
242:
The use of these names for the different multiplets can vary in literature. A chiral multiplet (whose highest component is a spinor) may sometimes be referred to as a
3290:
4880:
4087:
4008:
1884:
1864:
3319:
3165:
4632:
3744:
4931:
3598:
3578:
3134:
3114:
1998:
1924:
1904:
781:
4916:
4906:
4360:
1460:{\displaystyle {\bar {D}}_{\dot {\alpha }}=-{\bar {\partial }}_{\dot {\alpha }}-i\theta ^{\alpha }\sigma _{\alpha {\dot {\alpha }}}^{\mu }\partial _{\mu }.}
1526:
4885:
1632:
4926:
4429:
4936:
2493:{\displaystyle D_{\alpha }=\partial _{\alpha }+i\sigma _{\alpha {\dot {\alpha }}}^{\mu }{\bar {\theta }}^{\dot {\alpha }}\partial _{\mu }.}
4518:
Krippendorf, Sven; Quevedo, Fernando; Schlotterer, Oliver (5 November 2010). "Cambridge
Lectures on Supersymmetry and Extra Dimensions".
1054:
4625:
5052:
4941:
4665:
4979:
4974:
3622:
4911:
1788:
4618:
3747:
1214:. There exists a projection from the (full) superspace to chiral superspace. So, a function over chiral superspace can be
219:
supersymmetry for example), tensor multiplets and gravity multiplets. The highest component of a vector multiplet is a
4875:
4799:
1473:
1221:
306:
4959:
4844:
4660:
4372:
3753:
3260:
4859:
2559:
896:
288:
SUSY, a vector multiplet (whose highest component is a vector) can sometimes be referred to as a chiral multiplet.
4829:
4241:
1936:
1110:
4713:
3614:
115:
in a 1974 article. Operations on superfields and a partial classification were presented a few months later by
4854:
66:
3712:; this term has been abandoned, but the name "hypermultiplet" for some of its representations is still used.
1271:
4160:
5209:
4964:
4814:
4718:
4090:
2349:
1164:
910:
356:
249:
180:
138:
92:
62:
47:
4901:
4839:
4205:
2512:
4994:
4989:
4743:
4723:
3639:
3199:
1215:
232:
43:
4403:
4325:
4287:
4250:
4130:
4100:
3957:
3919:
3861:
3808:
3645:
2526:
2322:
1732:
1703:
1016:
955:
4779:
4728:
4547:
4485:
4409:
3720:
This section records some commonly used irreducible supermultiplets in extended supersymmetry in the
3172:
112:
39:
4046:
3895:
3837:
2609:
4999:
4984:
4969:
4738:
31:
5108:
4680:
4675:
4597:
4519:
4446:
96:
1307:
899:
supermultiplet, and so different constraints are needed to isolate irreducible representations.
3834:. For supermultiplets representing massless particles, on physical grounds the maximum allowed
4425:
4016:
3536:
3512:
3322:
3232:
1761:
989:
3269:
2503:
An antichiral superfield can be constructed as the complex conjugate of a chiral superfield.
4809:
4708:
4695:
4555:
4493:
4417:
4567:
4072:
3993:
1869:
1849:
5138:
5103:
4824:
4819:
4563:
4458:
3889:
3689:
3295:
3141:
5168:
3723:
4551:
4489:
4413:
3750:
construction in the sense that there is a vacuum vector annihilated by the supercharges
888:{\displaystyle \phi ,\chi ,{\bar {\chi }}',V_{\mu },F,{\bar {F}}',\xi ,{\bar {\xi }}',D}
5158:
5143:
4789:
3583:
3563:
3119:
3099:
1983:
1909:
1889:
116:
4473:
5203:
5183:
5163:
5113:
4748:
4685:
4655:
4641:
4578:
4559:
4497:
1619:{\displaystyle \Phi (y,\theta )=\phi (y)+{\sqrt {2}}\theta \psi (y)+\theta ^{2}F(y),}
1203:
236:
76:. It is a feature of supersymmetric field theories that particles form pairs, called
135:
The most commonly used supermultiplets are vector multiplets, chiral multiplets (in
5188:
5173:
5133:
5123:
5118:
5009:
4951:
4834:
4703:
4670:
4356:
4041:
3685:
3673:
3530:
124:
77:
5178:
5153:
5148:
5098:
5077:
5042:
5037:
4764:
4094:
4011:
3226:
220:
120:
108:
4421:
5082:
5072:
5057:
4849:
4769:
4733:
983:
58:
5128:
5032:
4921:
73:
4589:
17:
5067:
5062:
5047:
5022:
296:
Conventions in this section follow the notes by
Figueroa-O'Farrill (
228:
85:
4596:
Figueroa-O'Farrill, J. M. (2001). "Busstepp
Lectures on Supersymmetry".
2511:
For an action which can be defined from a single chiral superfield, see
1693:{\displaystyle y^{\mu }=x^{\mu }+i\theta \sigma ^{\mu }{\bar {\theta }}}
5027:
4602:
4804:
4794:
4382:
4377:
3601:
1933:
The field can then be expressed in terms of the original coordinates
1927:
1155:
224:
81:
2556:
A vector superfield (also known as a real superfield) is a function
1700:. The superfield is independent of the 'conjugate spin coordinates'
235:, although the organization of the fields as representations of the
3621:
is a vector multiplet containing d real scalars. Similarly, in an
1886:
is a Weyl spinor. There is also the auxiliary complex scalar field
1100:{\displaystyle \theta _{\alpha },{\bar {\theta }}^{\dot {\alpha }}}
5017:
4524:
3704:
The name "hypermultiplet" comes from old term "hypersymmetry" for
3618:
3259:
Their transformation properties and uses are further discussed in
4610:
4614:
4355:
contains one gauge field, four Weyl fermions, six scalars, and
4284:
consists of two Weyl fermions and two complex scalars, or two
3325:. In this gauge, the expansion takes on the much simpler form
91:
These supersymmetric fields are used to build supersymmetric
4331:
4293:
4256:
4136:
4106:
3963:
3925:
3901:
3867:
3843:
3818:
3790:
3651:
2532:
1182:
961:
928:
374:
267:
198:
156:
2312:, which is the complex conjugate of chiral superspace, and
223:, the highest component of a chiral or hypermultiplet is a
3580:
is an auxiliary scalar field. It is conventionally called
1333:
is the covariant derivative, given in index notation as
986:. Superspace contains the usual space-time coordinates
3672:
supersymmetry in 4 dimensions, containing two complex
3054:
3004:
2954:
2870:
2743:
2700:
1837:{\displaystyle {\bar {D}}_{\dot {\alpha }}y^{\mu }=0.}
297:
4472:
Ferrara, Sergio; Wess, Julius; Zumino, Bruno (1974).
4328:
4290:
4253:
4208:
4163:
4133:
4103:
4075:
4049:
4019:
3996:
3960:
3922:
3898:
3864:
3840:
3811:
3756:
3726:
3648:
3617:, while its dimensional reduction on a d-dimensional
3586:
3566:
3539:
3515:
3334:
3298:
3272:
3235:
3202:
3175:
3144:
3122:
3102:
2648:
2612:
2562:
2529:
2394:
2352:
2325:
2009:
1986:
1939:
1912:
1892:
1872:
1852:
1791:
1764:
1735:
1706:
1635:
1529:
1476:
1342:
1310:
1274:
1224:
1167:
1113:
1057:
1019:
992:
958:
913:
784:
404:
359:
309:
252:
231:. The names are defined so as to be invariant under
183:
141:
72:
Phenomenologically, superfields are used to describe
227:, the highest component of a gravity multiplet is a
5091:
5008:
4950:
4894:
4868:
4757:
4694:
4648:
4344:
4306:
4269:
4232:
4194:
4149:
4119:
4081:
4061:
4032:
4002:
3976:
3938:
3908:
3880:
3850:
3826:
3797:
3738:
3664:
3592:
3572:
3552:
3521:
3498:
3313:
3284:
3248:
3215:
3188:
3159:
3128:
3108:
3081:
2631:
2598:
2545:
2492:
2377:
2338:
2292:
1992:
1972:
1918:
1898:
1878:
1858:
1836:
1777:
1750:
1721:
1692:
1618:
1512:
1459:
1325:
1296:
1260:
1195:
1146:
1099:
1043:
1005:
974:
941:
907:A (anti-)chiral superfield is a supermultiplet of
887:
766:
387:
345:
280:
211:
169:
1513:{\displaystyle \Phi (x,\theta ,{\bar {\theta }})}
1261:{\displaystyle \Phi (x,\theta ,{\bar {\theta }})}
982:supersymmetry may be written using the notion of
346:{\displaystyle \Phi (x,\theta ,{\bar {\theta }})}
3798:{\displaystyle Q^{A},A=1,\cdots ,{\mathcal {N}}}
1930:which plays an important role in some theories.
177:supersymmetry for example), hypermultiplets (in
4538:Fayet, P. (1976), "Fermi-Bose hypersymmetry",
4097:). These can also be organised into a pair of
4626:
2599:{\displaystyle V(x,\theta ,{\bar {\theta }})}
2523:The vector superfield is a supermultiplet of
895:are different complex fields. This is not an
27:A representation of the supersymmetry algebra
8:
1973:{\displaystyle (x,\theta ,{\bar {\theta }})}
1147:{\displaystyle \alpha ,{\dot {\alpha }}=1,2}
4586:N=2 supersymmetric dynamics for pedestrians
3638:is a type of representation of an extended
4633:
4619:
4611:
1846:The expansion has the interpretation that
4601:
4523:
4330:
4329:
4327:
4292:
4291:
4289:
4255:
4254:
4252:
4240:. Such a multiplet can be used to define
4207:
4177:
4162:
4135:
4134:
4132:
4105:
4104:
4102:
4074:
4048:
4024:
4018:
3995:
3962:
3961:
3959:
3924:
3923:
3921:
3900:
3899:
3897:
3866:
3865:
3863:
3842:
3841:
3839:
3817:
3816:
3810:
3789:
3788:
3761:
3755:
3725:
3650:
3649:
3647:
3585:
3565:
3544:
3538:
3514:
3484:
3473:
3472:
3465:
3451:
3436:
3425:
3424:
3409:
3408:
3397:
3396:
3390:
3377:
3362:
3361:
3355:
3339:
3333:
3297:
3271:
3240:
3234:
3207:
3201:
3180:
3174:
3143:
3121:
3101:
3053:
3036:
3026:
3019:
3003:
2985:
2979:
2969:
2953:
2933:
2923:
2902:
2892:
2882:
2869:
2856:
2841:
2835:
2819:
2805:
2799:
2760:
2754:
2742:
2715:
2699:
2686:
2676:
2647:
2623:
2611:
2582:
2581:
2561:
2531:
2530:
2528:
2481:
2465:
2464:
2453:
2452:
2445:
2433:
2432:
2428:
2412:
2399:
2393:
2360:
2351:
2330:
2324:
2266:
2255:
2254:
2247:
2233:
2219:
2218:
2212:
2190:
2180:
2164:
2143:
2128:
2127:
2121:
2090:
2061:
2029:
2028:
2008:
1985:
1956:
1955:
1938:
1911:
1891:
1871:
1851:
1822:
1806:
1805:
1794:
1793:
1790:
1769:
1763:
1737:
1736:
1734:
1708:
1707:
1705:
1679:
1678:
1672:
1653:
1640:
1634:
1595:
1566:
1528:
1496:
1495:
1475:
1448:
1438:
1426:
1425:
1421:
1411:
1389:
1388:
1377:
1376:
1357:
1356:
1345:
1344:
1341:
1312:
1311:
1309:
1275:
1273:
1244:
1243:
1223:
1181:
1180:
1166:
1154:, transforming as a two-component (Weyl)
1121:
1120:
1112:
1085:
1084:
1073:
1072:
1062:
1056:
1018:
997:
991:
960:
959:
957:
927:
926:
912:
864:
863:
838:
837:
821:
799:
798:
783:
746:
735:
734:
727:
696:
695:
683:
682:
676:
648:
637:
636:
608:
607:
600:
589:
588:
566:
544:
531:
516:
515:
488:
487:
475:
474:
424:
423:
403:
373:
372:
358:
329:
328:
308:
292:Superfields in d = 4, N = 1 supersymmetry
266:
265:
251:
197:
196:
182:
155:
154:
140:
4402:Salam, Abdus; Strathdee, J. (May 1994).
3642:, in particular the matter multiplet of
3266:Using gauge transformations, the fields
1218:to the full superspace. Such a function
4474:"Supergauge multiplets and superfields"
4394:
1051:, and four extra fermionic coordinates
4454:
4444:
4361:N = 4 supersymmetric YangâMills theory
2606:which satisfies the reality condition
1297:{\displaystyle {\overline {D}}\Phi =0}
4195:{\displaystyle W=(A_{\mu },\lambda )}
3709:
3321:can be set to zero. This is known as
7:
2639:. Such a field admits the expansion
2378:{\displaystyle D\Phi ^{\dagger }=0,}
1196:{\displaystyle d=4,{\mathcal {N}}=1}
942:{\displaystyle d=4,{\mathcal {N}}=1}
388:{\displaystyle d=4,{\mathcal {N}}=1}
281:{\displaystyle d=4,{\mathcal {N}}=2}
212:{\displaystyle d=4,{\mathcal {N}}=2}
170:{\displaystyle d=4,{\mathcal {N}}=1}
4233:{\displaystyle \Phi =(\phi ,\psi )}
1980:by substituting the expression for
1268:satisfies the covariant constraint
95:, where the fields are promoted to
4209:
3997:
3216:{\displaystyle \lambda ^{\alpha }}
2976:
2899:
2478:
2409:
2357:
2327:
2187:
2140:
2010:
1530:
1477:
1445:
1379:
1285:
1225:
405:
310:
25:
4408:. Vol. 5. pp. 404â409.
3746:case. These are constructed by a
3716:Extended supersymmetry (N > 1)
395:supersymmetry can be expanded as
4666:Supersymmetric quantum mechanics
4345:{\displaystyle {\mathcal {N}}=4}
4307:{\displaystyle {\mathcal {N}}=1}
4270:{\displaystyle {\mathcal {N}}=2}
4150:{\displaystyle {\mathcal {N}}=1}
4120:{\displaystyle {\mathcal {N}}=1}
3977:{\displaystyle {\mathcal {N}}=2}
3939:{\displaystyle {\mathcal {N}}=4}
3881:{\displaystyle {\mathcal {N}}=8}
3827:{\displaystyle 2^{\mathcal {N}}}
3665:{\displaystyle {\mathcal {N}}=2}
2546:{\displaystyle {\mathcal {N}}=1}
2339:{\displaystyle \Phi ^{\dagger }}
1751:{\displaystyle {\bar {\theta }}}
1729:in the sense that it depends on
1722:{\displaystyle {\bar {\theta }}}
1044:{\displaystyle \mu =0,\ldots ,3}
975:{\displaystyle {\mathcal {N}}=1}
952:In four dimensions, the minimal
67:associated supermultiplet bundle
3189:{\displaystyle \chi _{\alpha }}
2507:Actions from chiral superfields
107:Superfields were introduced by
4227:
4215:
4189:
4170:
4062:{\displaystyle \lambda ,\psi }
3909:{\displaystyle {\mathcal {N}}}
3851:{\displaystyle {\mathcal {N}}}
3478:
3430:
3414:
3402:
3367:
2786:
2771:
2736:
2721:
2632:{\displaystyle V=V^{\dagger }}
2593:
2587:
2566:
2458:
2284:
2278:
2260:
2224:
2205:
2199:
2158:
2152:
2133:
2105:
2099:
2080:
2074:
2055:
2049:
2040:
2034:
2013:
1967:
1961:
1940:
1799:
1742:
1713:
1684:
1610:
1604:
1585:
1579:
1560:
1554:
1545:
1533:
1507:
1501:
1480:
1382:
1350:
1317:
1255:
1249:
1228:
1078:
869:
843:
804:
761:
755:
740:
717:
711:
701:
688:
666:
660:
642:
629:
623:
613:
594:
581:
575:
556:
550:
521:
509:
503:
493:
480:
468:
462:
450:
444:
435:
429:
408:
340:
334:
313:
1:
4089:(which also transform in the
3748:highest-weight representation
303:A general complex superfield
4560:10.1016/0550-3213(76)90458-2
4498:10.1016/0370-2693(74)90283-4
4359:conjugates. This appears in
3805:. The irreps have dimension
3031:
2990:
2928:
2887:
2861:
2846:
2810:
2766:
2691:
2681:
1280:
4661:Supersymmetric gauge theory
4405:Super-Gauge Transformations
4373:Supersymmetric gauge theory
3261:supersymmetric gauge theory
3092:The constituent fields are
1926:by convention: this is the
1866:is a complex scalar field,
5226:
4960:Pure 4D N = 1 supergravity
4422:10.1142/9789812795915_0047
1326:{\displaystyle {\bar {D}}}
4860:Electricâmagnetic duality
3708:=2 supersymmetry used by
2319:An antichiral superfield
2308:Similarly, there is also
1785:. It can be checked that
131:Naming and classification
4881:HaagâĆopuszaĆskiâSohnius
4855:Little hierarchy problem
4033:{\displaystyle A_{\mu }}
3553:{\displaystyle A_{\mu }}
3522:{\displaystyle \lambda }
3249:{\displaystyle A_{\mu }}
1778:{\displaystyle y^{\mu }}
1520:can then be expanded as
1006:{\displaystyle x^{\mu }}
4937:6D (2,0) superconformal
3285:{\displaystyle C,\chi }
3169:Two Weyl spinor fields
3138:A complex scalar field
3096:Two real scalar fields
4917:N = 4 super YangâMills
4907:N = 1 super YangâMills
4815:Supersymmetry breaking
4719:Superconformal algebra
4714:Super-Poincaré algebra
4575:A Supersymmetry Primer
4346:
4308:
4271:
4234:
4196:
4151:
4121:
4091:adjoint representation
4083:
4063:
4034:
4004:
3978:
3940:
3910:
3892:, the maximum allowed
3882:
3852:
3828:
3799:
3740:
3666:
3600:, and is known as the
3594:
3574:
3554:
3523:
3500:
3315:
3286:
3250:
3217:
3190:
3161:
3130:
3110:
3083:
2633:
2600:
2547:
2494:
2379:
2340:
2314:antichiral superfields
2304:Antichiral superfields
2294:
1994:
1974:
1920:
1900:
1880:
1860:
1838:
1779:
1752:
1723:
1694:
1620:
1514:
1461:
1327:
1298:
1262:
1197:
1148:
1101:
1045:
1007:
976:
943:
889:
768:
389:
347:
282:
213:
171:
93:quantum field theories
48:extended supersymmetry
4995:Type IIB supergravity
4990:Type IIA supergravity
4965:4D N = 1 supergravity
4830:SeibergâWitten theory
4744:Super Minkowski space
4724:Supersymmetry algebra
4347:
4309:
4272:
4242:SeibergâWitten theory
4235:
4202:and chiral multiplet
4197:
4152:
4122:
4084:
4082:{\displaystyle \phi }
4064:
4035:
4005:
4003:{\displaystyle \Psi }
3979:
3941:
3911:
3883:
3853:
3829:
3800:
3741:
3667:
3640:supersymmetry algebra
3623:11-dimensional theory
3595:
3575:
3555:
3524:
3501:
3316:
3287:
3251:
3225:A real vector field (
3218:
3191:
3162:
3131:
3111:
3084:
2634:
2601:
2548:
2495:
2380:
2341:
2310:antichiral superspace
2295:
1995:
1975:
1921:
1901:
1881:
1879:{\displaystyle \psi }
1861:
1859:{\displaystyle \phi }
1839:
1780:
1753:
1724:
1695:
1621:
1515:
1462:
1328:
1299:
1263:
1198:
1149:
1102:
1046:
1008:
977:
944:
890:
769:
390:
348:
283:
233:dimensional reduction
214:
172:
44:supersymmetry algebra
4780:Short supermultiplet
4579:arXiv:hep-ph/9709356
4326:
4288:
4251:
4206:
4161:
4131:
4101:
4073:
4047:
4017:
3994:
3958:
3920:
3896:
3862:
3838:
3809:
3754:
3724:
3646:
3615:MajoranaâWeyl spinor
3584:
3564:
3537:
3513:
3332:
3314:{\displaystyle M+iN}
3296:
3270:
3233:
3200:
3173:
3160:{\displaystyle M+iN}
3142:
3120:
3100:
2646:
2610:
2560:
2527:
2392:
2350:
2323:
2007:
1984:
1937:
1910:
1890:
1870:
1850:
1789:
1762:
1733:
1704:
1633:
1527:
1474:
1470:A chiral superfield
1340:
1308:
1272:
1222:
1165:
1111:
1055:
1017:
990:
956:
911:
782:
402:
357:
307:
250:
181:
139:
5000:Gauged supergravity
4985:Type I supergravity
4942:ABJM superconformal
4739:Harmonic superspace
4573:Stephen P. Martin.
4552:1976NuPhB.113..135F
4490:1974PhLB...51..239F
4414:1994spas.book..404S
4314:chiral multiplets.
3739:{\displaystyle d=4}
3688:Ï, and two further
2450:
1443:
1210:is a function over
1158:and its conjugate.
32:theoretical physics
4975:Higher dimensional
4970:N = 8 supergravity
4886:Nonrenormalization
4681:Super vector space
4676:Superstring theory
4342:
4304:
4267:
4230:
4192:
4147:
4117:
4079:
4059:
4030:
4000:
3974:
3936:
3906:
3878:
3848:
3824:
3795:
3736:
3662:
3590:
3570:
3550:
3519:
3496:
3311:
3282:
3246:
3213:
3186:
3157:
3126:
3106:
3079:
3063:
3013:
2963:
2879:
2752:
2709:
2629:
2596:
2543:
2490:
2424:
2375:
2336:
2290:
1990:
1970:
1916:
1896:
1876:
1856:
1834:
1775:
1748:
1719:
1690:
1616:
1510:
1457:
1417:
1323:
1294:
1258:
1193:
1144:
1097:
1041:
1003:
972:
939:
885:
764:
385:
343:
278:
209:
167:
5197:
5196:
4840:WessâZumino gauge
4540:Nuclear Physics B
4431:978-981-02-1662-7
4157:vector multiplet
3890:renormalizability
3593:{\displaystyle D}
3573:{\displaystyle D}
3481:
3459:
3433:
3417:
3405:
3370:
3342:
3323:Wess-Zumino gauge
3129:{\displaystyle D}
3109:{\displaystyle C}
3062:
3034:
3012:
2993:
2962:
2931:
2890:
2878:
2864:
2849:
2813:
2769:
2751:
2708:
2694:
2684:
2590:
2519:Vector superfield
2513:WessâZumino model
2473:
2461:
2441:
2263:
2241:
2227:
2174:
2173:
2136:
2066:
2037:
1993:{\displaystyle y}
1964:
1919:{\displaystyle F}
1899:{\displaystyle F}
1814:
1802:
1745:
1716:
1687:
1571:
1504:
1434:
1397:
1385:
1365:
1353:
1320:
1283:
1252:
1212:chiral superspace
1208:chiral superfield
1129:
1093:
1081:
903:Chiral superfield
872:
846:
807:
743:
704:
691:
645:
616:
597:
524:
496:
483:
432:
337:
16:(Redirected from
5217:
4980:11D supergravity
4709:Lie superalgebra
4696:Supermathematics
4635:
4628:
4621:
4612:
4607:
4605:
4584:Yuji Tachikawa.
4570:
4530:
4529:
4527:
4515:
4509:
4508:
4506:
4504:
4469:
4463:
4462:
4456:
4452:
4450:
4442:
4440:
4438:
4399:
4353:vector multiplet
4351:
4349:
4348:
4343:
4335:
4334:
4313:
4311:
4310:
4305:
4297:
4296:
4282:scalar multiplet
4276:
4274:
4273:
4268:
4260:
4259:
4239:
4237:
4236:
4231:
4201:
4199:
4198:
4193:
4182:
4181:
4156:
4154:
4153:
4148:
4140:
4139:
4126:
4124:
4123:
4118:
4110:
4109:
4088:
4086:
4085:
4080:
4068:
4066:
4065:
4060:
4039:
4037:
4036:
4031:
4029:
4028:
4009:
4007:
4006:
4001:
3989:chiral multiplet
3983:
3981:
3980:
3975:
3967:
3966:
3945:
3943:
3942:
3937:
3929:
3928:
3915:
3913:
3912:
3907:
3905:
3904:
3887:
3885:
3884:
3879:
3871:
3870:
3857:
3855:
3854:
3849:
3847:
3846:
3833:
3831:
3830:
3825:
3823:
3822:
3821:
3804:
3802:
3801:
3796:
3794:
3793:
3766:
3765:
3745:
3743:
3742:
3737:
3692:complex scalars
3671:
3669:
3668:
3663:
3655:
3654:
3599:
3597:
3596:
3591:
3579:
3577:
3576:
3571:
3559:
3557:
3556:
3551:
3549:
3548:
3528:
3526:
3525:
3520:
3505:
3503:
3502:
3497:
3489:
3488:
3483:
3482:
3474:
3470:
3469:
3460:
3452:
3441:
3440:
3435:
3434:
3426:
3419:
3418:
3410:
3407:
3406:
3398:
3395:
3394:
3382:
3381:
3372:
3371:
3363:
3360:
3359:
3344:
3343:
3340:
3320:
3318:
3317:
3312:
3291:
3289:
3288:
3283:
3255:
3253:
3252:
3247:
3245:
3244:
3222:
3220:
3219:
3214:
3212:
3211:
3195:
3193:
3192:
3187:
3185:
3184:
3166:
3164:
3163:
3158:
3135:
3133:
3132:
3127:
3115:
3113:
3112:
3107:
3088:
3086:
3085:
3080:
3075:
3071:
3064:
3055:
3041:
3040:
3035:
3027:
3024:
3023:
3014:
3005:
2999:
2995:
2994:
2986:
2984:
2983:
2974:
2973:
2964:
2955:
2938:
2937:
2932:
2924:
2915:
2911:
2907:
2906:
2897:
2896:
2891:
2883:
2880:
2871:
2865:
2857:
2850:
2842:
2840:
2839:
2824:
2823:
2814:
2806:
2804:
2803:
2770:
2765:
2764:
2755:
2753:
2744:
2720:
2719:
2710:
2701:
2695:
2687:
2685:
2677:
2638:
2636:
2635:
2630:
2628:
2627:
2605:
2603:
2602:
2597:
2592:
2591:
2583:
2552:
2550:
2549:
2544:
2536:
2535:
2499:
2497:
2496:
2491:
2486:
2485:
2476:
2475:
2474:
2466:
2463:
2462:
2454:
2449:
2444:
2443:
2442:
2434:
2417:
2416:
2404:
2403:
2384:
2382:
2381:
2376:
2365:
2364:
2345:
2343:
2342:
2337:
2335:
2334:
2299:
2297:
2296:
2291:
2271:
2270:
2265:
2264:
2256:
2252:
2251:
2242:
2234:
2229:
2228:
2220:
2217:
2216:
2195:
2194:
2185:
2184:
2175:
2169:
2165:
2148:
2147:
2138:
2137:
2129:
2126:
2125:
2095:
2094:
2067:
2062:
2039:
2038:
2030:
1999:
1997:
1996:
1991:
1979:
1977:
1976:
1971:
1966:
1965:
1957:
1925:
1923:
1922:
1917:
1905:
1903:
1902:
1897:
1885:
1883:
1882:
1877:
1865:
1863:
1862:
1857:
1843:
1841:
1840:
1835:
1827:
1826:
1817:
1816:
1815:
1807:
1804:
1803:
1795:
1784:
1782:
1781:
1776:
1774:
1773:
1757:
1755:
1754:
1749:
1747:
1746:
1738:
1728:
1726:
1725:
1720:
1718:
1717:
1709:
1699:
1697:
1696:
1691:
1689:
1688:
1680:
1677:
1676:
1658:
1657:
1645:
1644:
1625:
1623:
1622:
1617:
1600:
1599:
1572:
1567:
1519:
1517:
1516:
1511:
1506:
1505:
1497:
1466:
1464:
1463:
1458:
1453:
1452:
1442:
1437:
1436:
1435:
1427:
1416:
1415:
1400:
1399:
1398:
1390:
1387:
1386:
1378:
1368:
1367:
1366:
1358:
1355:
1354:
1346:
1332:
1330:
1329:
1324:
1322:
1321:
1313:
1303:
1301:
1300:
1295:
1284:
1276:
1267:
1265:
1264:
1259:
1254:
1253:
1245:
1202:
1200:
1199:
1194:
1186:
1185:
1153:
1151:
1150:
1145:
1131:
1130:
1122:
1106:
1104:
1103:
1098:
1096:
1095:
1094:
1086:
1083:
1082:
1074:
1067:
1066:
1050:
1048:
1047:
1042:
1012:
1010:
1009:
1004:
1002:
1001:
981:
979:
978:
973:
965:
964:
948:
946:
945:
940:
932:
931:
894:
892:
891:
886:
878:
874:
873:
865:
852:
848:
847:
839:
826:
825:
813:
809:
808:
800:
773:
771:
770:
765:
751:
750:
745:
744:
736:
732:
731:
710:
706:
705:
697:
693:
692:
684:
681:
680:
653:
652:
647:
646:
638:
622:
618:
617:
609:
605:
604:
599:
598:
590:
571:
570:
549:
548:
536:
535:
526:
525:
517:
502:
498:
497:
489:
485:
484:
476:
434:
433:
425:
394:
392:
391:
386:
378:
377:
352:
350:
349:
344:
339:
338:
330:
287:
285:
284:
279:
271:
270:
244:scalar multiplet
218:
216:
215:
210:
202:
201:
176:
174:
173:
168:
160:
159:
84:are paired with
46:, possibly with
21:
5225:
5224:
5220:
5219:
5218:
5216:
5215:
5214:
5200:
5199:
5198:
5193:
5087:
5004:
4946:
4890:
4876:ColemanâMandula
4864:
4825:Seiberg duality
4820:Konishi anomaly
4753:
4690:
4644:
4639:
4595:
4590:arXiv:1312.2684
4537:
4534:
4533:
4517:
4516:
4512:
4502:
4500:
4471:
4470:
4466:
4453:
4443:
4436:
4434:
4432:
4401:
4400:
4396:
4391:
4369:
4324:
4323:
4320:
4286:
4285:
4249:
4248:
4204:
4203:
4173:
4159:
4158:
4129:
4128:
4127:multiplets, an
4099:
4098:
4071:
4070:
4069:, and a scalar
4045:
4044:
4020:
4015:
4014:
3992:
3991:
3956:
3955:
3952:
3918:
3917:
3894:
3893:
3860:
3859:
3836:
3835:
3812:
3807:
3806:
3757:
3752:
3751:
3722:
3721:
3718:
3700:
3683:
3644:
3643:
3632:
3610:
3582:
3581:
3562:
3561:
3540:
3535:
3534:
3511:
3510:
3471:
3461:
3423:
3386:
3373:
3351:
3335:
3330:
3329:
3294:
3293:
3268:
3267:
3236:
3231:
3230:
3203:
3198:
3197:
3176:
3171:
3170:
3140:
3139:
3118:
3117:
3098:
3097:
3046:
3042:
3025:
3015:
2975:
2965:
2946:
2942:
2922:
2898:
2881:
2855:
2851:
2831:
2815:
2795:
2756:
2711:
2644:
2643:
2619:
2608:
2607:
2558:
2557:
2553:supersymmetry.
2525:
2524:
2521:
2509:
2477:
2451:
2408:
2395:
2390:
2389:
2356:
2348:
2347:
2326:
2321:
2320:
2306:
2253:
2243:
2208:
2186:
2176:
2139:
2117:
2086:
2005:
2004:
1982:
1981:
1935:
1934:
1908:
1907:
1888:
1887:
1868:
1867:
1848:
1847:
1818:
1792:
1787:
1786:
1765:
1760:
1759:
1731:
1730:
1702:
1701:
1668:
1649:
1636:
1631:
1630:
1591:
1525:
1524:
1472:
1471:
1444:
1407:
1375:
1343:
1338:
1337:
1306:
1305:
1270:
1269:
1220:
1219:
1163:
1162:
1109:
1108:
1071:
1058:
1053:
1052:
1015:
1014:
993:
988:
987:
954:
953:
949:supersymmetry.
909:
908:
905:
862:
836:
817:
797:
780:
779:
733:
723:
694:
672:
635:
606:
587:
562:
540:
527:
486:
400:
399:
355:
354:
305:
304:
294:
248:
247:
179:
178:
137:
136:
133:
113:J. A. Strathdee
105:
28:
23:
22:
15:
12:
11:
5:
5223:
5221:
5213:
5212:
5202:
5201:
5195:
5194:
5192:
5191:
5186:
5181:
5176:
5171:
5166:
5161:
5156:
5151:
5146:
5141:
5136:
5131:
5126:
5121:
5116:
5111:
5106:
5101:
5095:
5093:
5089:
5088:
5086:
5085:
5080:
5075:
5070:
5065:
5060:
5055:
5050:
5045:
5040:
5035:
5030:
5025:
5020:
5014:
5012:
5006:
5005:
5003:
5002:
4997:
4992:
4987:
4982:
4977:
4972:
4967:
4962:
4956:
4954:
4948:
4947:
4945:
4944:
4939:
4934:
4929:
4924:
4919:
4914:
4909:
4904:
4898:
4896:
4895:Field theories
4892:
4891:
4889:
4888:
4883:
4878:
4872:
4870:
4866:
4865:
4863:
4862:
4857:
4852:
4847:
4842:
4837:
4832:
4827:
4822:
4817:
4812:
4807:
4802:
4797:
4792:
4790:Superpotential
4787:
4782:
4777:
4775:Supermultiplet
4772:
4767:
4761:
4759:
4755:
4754:
4752:
4751:
4746:
4741:
4736:
4731:
4726:
4721:
4716:
4711:
4706:
4700:
4698:
4692:
4691:
4689:
4688:
4683:
4678:
4673:
4668:
4663:
4658:
4652:
4650:
4649:General topics
4646:
4645:
4640:
4638:
4637:
4630:
4623:
4615:
4609:
4608:
4603:hep-th/0109172
4593:
4582:
4571:
4546:(1): 135â155,
4532:
4531:
4510:
4484:(3): 239â241.
4464:
4455:|journal=
4430:
4393:
4392:
4390:
4387:
4386:
4385:
4380:
4375:
4368:
4365:
4341:
4338:
4333:
4319:
4316:
4303:
4300:
4295:
4278:hypermultiplet
4266:
4263:
4258:
4229:
4226:
4223:
4220:
4217:
4214:
4211:
4191:
4188:
4185:
4180:
4176:
4172:
4169:
4166:
4146:
4143:
4138:
4116:
4113:
4108:
4078:
4058:
4055:
4052:
4027:
4023:
3999:
3973:
3970:
3965:
3951:
3948:
3935:
3932:
3927:
3903:
3877:
3874:
3869:
3845:
3820:
3815:
3792:
3787:
3784:
3781:
3778:
3775:
3772:
3769:
3764:
3760:
3735:
3732:
3729:
3717:
3714:
3696:
3679:
3661:
3658:
3653:
3636:hypermultiplet
3631:
3630:Hypermultiplet
3628:
3609:
3606:
3589:
3569:
3547:
3543:
3518:
3507:
3506:
3495:
3492:
3487:
3480:
3477:
3468:
3464:
3458:
3455:
3450:
3447:
3444:
3439:
3432:
3429:
3422:
3416:
3413:
3404:
3401:
3393:
3389:
3385:
3380:
3376:
3369:
3366:
3358:
3354:
3350:
3347:
3338:
3310:
3307:
3304:
3301:
3281:
3278:
3275:
3257:
3256:
3243:
3239:
3223:
3210:
3206:
3183:
3179:
3167:
3156:
3153:
3150:
3147:
3136:
3125:
3105:
3090:
3089:
3078:
3074:
3070:
3067:
3061:
3058:
3052:
3049:
3045:
3039:
3033:
3030:
3022:
3018:
3011:
3008:
3002:
2998:
2992:
2989:
2982:
2978:
2972:
2968:
2961:
2958:
2952:
2949:
2945:
2941:
2936:
2930:
2927:
2921:
2918:
2914:
2910:
2905:
2901:
2895:
2889:
2886:
2877:
2874:
2868:
2863:
2860:
2854:
2848:
2845:
2838:
2834:
2830:
2827:
2822:
2818:
2812:
2809:
2802:
2798:
2794:
2791:
2788:
2785:
2782:
2779:
2776:
2773:
2768:
2763:
2759:
2750:
2747:
2741:
2738:
2735:
2732:
2729:
2726:
2723:
2718:
2714:
2707:
2704:
2698:
2693:
2690:
2683:
2680:
2675:
2672:
2669:
2666:
2663:
2660:
2657:
2654:
2651:
2626:
2622:
2618:
2615:
2595:
2589:
2586:
2580:
2577:
2574:
2571:
2568:
2565:
2542:
2539:
2534:
2520:
2517:
2508:
2505:
2501:
2500:
2489:
2484:
2480:
2472:
2469:
2460:
2457:
2448:
2440:
2437:
2431:
2427:
2423:
2420:
2415:
2411:
2407:
2402:
2398:
2374:
2371:
2368:
2363:
2359:
2355:
2333:
2329:
2305:
2302:
2301:
2300:
2289:
2286:
2283:
2280:
2277:
2274:
2269:
2262:
2259:
2250:
2246:
2240:
2237:
2232:
2226:
2223:
2215:
2211:
2207:
2204:
2201:
2198:
2193:
2189:
2183:
2179:
2172:
2168:
2163:
2160:
2157:
2154:
2151:
2146:
2142:
2135:
2132:
2124:
2120:
2116:
2113:
2110:
2107:
2104:
2101:
2098:
2093:
2089:
2085:
2082:
2079:
2076:
2073:
2070:
2065:
2060:
2057:
2054:
2051:
2048:
2045:
2042:
2036:
2033:
2027:
2024:
2021:
2018:
2015:
2012:
1989:
1969:
1963:
1960:
1954:
1951:
1948:
1945:
1942:
1915:
1895:
1875:
1855:
1833:
1830:
1825:
1821:
1813:
1810:
1801:
1798:
1772:
1768:
1744:
1741:
1715:
1712:
1686:
1683:
1675:
1671:
1667:
1664:
1661:
1656:
1652:
1648:
1643:
1639:
1627:
1626:
1615:
1612:
1609:
1606:
1603:
1598:
1594:
1590:
1587:
1584:
1581:
1578:
1575:
1570:
1565:
1562:
1559:
1556:
1553:
1550:
1547:
1544:
1541:
1538:
1535:
1532:
1509:
1503:
1500:
1494:
1491:
1488:
1485:
1482:
1479:
1468:
1467:
1456:
1451:
1447:
1441:
1433:
1430:
1424:
1420:
1414:
1410:
1406:
1403:
1396:
1393:
1384:
1381:
1374:
1371:
1364:
1361:
1352:
1349:
1319:
1316:
1293:
1290:
1287:
1282:
1279:
1257:
1251:
1248:
1242:
1239:
1236:
1233:
1230:
1227:
1192:
1189:
1184:
1179:
1176:
1173:
1170:
1143:
1140:
1137:
1134:
1128:
1125:
1119:
1116:
1092:
1089:
1080:
1077:
1070:
1065:
1061:
1040:
1037:
1034:
1031:
1028:
1025:
1022:
1000:
996:
971:
968:
963:
938:
935:
930:
925:
922:
919:
916:
904:
901:
884:
881:
877:
871:
868:
861:
858:
855:
851:
845:
842:
835:
832:
829:
824:
820:
816:
812:
806:
803:
796:
793:
790:
787:
776:
775:
763:
760:
757:
754:
749:
742:
739:
730:
726:
722:
719:
716:
713:
709:
703:
700:
690:
687:
679:
675:
671:
668:
665:
662:
659:
656:
651:
644:
641:
634:
631:
628:
625:
621:
615:
612:
603:
596:
593:
586:
583:
580:
577:
574:
569:
565:
561:
558:
555:
552:
547:
543:
539:
534:
530:
523:
520:
514:
511:
508:
505:
501:
495:
492:
482:
479:
473:
470:
467:
464:
461:
458:
455:
452:
449:
446:
443:
440:
437:
431:
428:
422:
419:
416:
413:
410:
407:
384:
381:
376:
371:
368:
365:
362:
342:
336:
333:
327:
324:
321:
318:
315:
312:
293:
290:
277:
274:
269:
264:
261:
258:
255:
208:
205:
200:
195:
192:
189:
186:
166:
163:
158:
153:
150:
147:
144:
132:
129:
117:Sergio Ferrara
104:
101:
57:is a field on
40:representation
36:supermultiplet
26:
24:
14:
13:
10:
9:
6:
4:
3:
2:
5222:
5211:
5210:Supersymmetry
5208:
5207:
5205:
5190:
5187:
5185:
5182:
5180:
5177:
5175:
5172:
5170:
5167:
5165:
5162:
5160:
5157:
5155:
5152:
5150:
5147:
5145:
5142:
5140:
5137:
5135:
5132:
5130:
5127:
5125:
5122:
5120:
5117:
5115:
5112:
5110:
5107:
5105:
5102:
5100:
5097:
5096:
5094:
5090:
5084:
5081:
5079:
5076:
5074:
5071:
5069:
5066:
5064:
5061:
5059:
5056:
5054:
5051:
5049:
5046:
5044:
5041:
5039:
5036:
5034:
5031:
5029:
5026:
5024:
5021:
5019:
5016:
5015:
5013:
5011:
5010:Superpartners
5007:
5001:
4998:
4996:
4993:
4991:
4988:
4986:
4983:
4981:
4978:
4976:
4973:
4971:
4968:
4966:
4963:
4961:
4958:
4957:
4955:
4953:
4949:
4943:
4940:
4938:
4935:
4933:
4930:
4928:
4925:
4923:
4920:
4918:
4915:
4913:
4910:
4908:
4905:
4903:
4900:
4899:
4897:
4893:
4887:
4884:
4882:
4879:
4877:
4874:
4873:
4871:
4867:
4861:
4858:
4856:
4853:
4851:
4848:
4846:
4843:
4841:
4838:
4836:
4833:
4831:
4828:
4826:
4823:
4821:
4818:
4816:
4813:
4811:
4808:
4806:
4803:
4801:
4798:
4796:
4793:
4791:
4788:
4786:
4783:
4781:
4778:
4776:
4773:
4771:
4768:
4766:
4763:
4762:
4760:
4756:
4750:
4749:Supermanifold
4747:
4745:
4742:
4740:
4737:
4735:
4732:
4730:
4727:
4725:
4722:
4720:
4717:
4715:
4712:
4710:
4707:
4705:
4702:
4701:
4699:
4697:
4693:
4687:
4686:Supergeometry
4684:
4682:
4679:
4677:
4674:
4672:
4669:
4667:
4664:
4662:
4659:
4657:
4656:Supersymmetry
4654:
4653:
4651:
4647:
4643:
4642:Supersymmetry
4636:
4631:
4629:
4624:
4622:
4617:
4616:
4613:
4604:
4599:
4594:
4591:
4587:
4583:
4580:
4576:
4572:
4569:
4565:
4561:
4557:
4553:
4549:
4545:
4541:
4536:
4535:
4526:
4521:
4514:
4511:
4499:
4495:
4491:
4487:
4483:
4479:
4478:Phys. Lett. B
4475:
4468:
4465:
4460:
4448:
4433:
4427:
4423:
4419:
4415:
4411:
4407:
4406:
4398:
4395:
4388:
4384:
4381:
4379:
4376:
4374:
4371:
4370:
4366:
4364:
4362:
4358:
4354:
4339:
4336:
4317:
4315:
4301:
4298:
4283:
4279:
4264:
4261:
4245:
4243:
4224:
4221:
4218:
4212:
4186:
4183:
4178:
4174:
4167:
4164:
4144:
4141:
4114:
4111:
4096:
4092:
4076:
4056:
4053:
4050:
4043:
4042:Weyl fermions
4025:
4021:
4013:
3990:
3986:
3971:
3968:
3949:
3947:
3933:
3930:
3891:
3875:
3872:
3813:
3785:
3782:
3779:
3776:
3773:
3770:
3767:
3762:
3758:
3749:
3733:
3730:
3727:
3715:
3713:
3711:
3707:
3702:
3699:
3695:
3691:
3687:
3682:
3678:
3675:
3659:
3656:
3641:
3637:
3629:
3627:
3624:
3620:
3616:
3607:
3605:
3603:
3587:
3567:
3545:
3541:
3532:
3516:
3493:
3490:
3485:
3475:
3466:
3462:
3456:
3453:
3448:
3445:
3442:
3437:
3427:
3420:
3411:
3399:
3391:
3387:
3383:
3378:
3374:
3364:
3356:
3352:
3348:
3345:
3336:
3328:
3327:
3326:
3324:
3308:
3305:
3302:
3299:
3279:
3276:
3273:
3264:
3262:
3241:
3237:
3228:
3224:
3208:
3204:
3181:
3177:
3168:
3154:
3151:
3148:
3145:
3137:
3123:
3103:
3095:
3094:
3093:
3076:
3072:
3068:
3065:
3059:
3056:
3050:
3047:
3043:
3037:
3028:
3020:
3016:
3009:
3006:
3000:
2996:
2987:
2980:
2970:
2966:
2959:
2956:
2950:
2947:
2943:
2939:
2934:
2925:
2919:
2916:
2912:
2908:
2903:
2893:
2884:
2875:
2872:
2866:
2858:
2852:
2843:
2836:
2832:
2828:
2825:
2820:
2816:
2807:
2800:
2796:
2792:
2789:
2783:
2780:
2777:
2774:
2761:
2757:
2748:
2745:
2739:
2733:
2730:
2727:
2724:
2716:
2712:
2705:
2702:
2696:
2688:
2678:
2673:
2670:
2667:
2664:
2661:
2658:
2655:
2652:
2649:
2642:
2641:
2640:
2624:
2620:
2616:
2613:
2584:
2578:
2575:
2572:
2569:
2563:
2554:
2540:
2537:
2518:
2516:
2514:
2506:
2504:
2487:
2482:
2470:
2467:
2455:
2446:
2438:
2435:
2429:
2425:
2421:
2418:
2413:
2405:
2400:
2396:
2388:
2387:
2386:
2372:
2369:
2366:
2361:
2353:
2331:
2317:
2315:
2311:
2303:
2287:
2281:
2275:
2272:
2267:
2257:
2248:
2244:
2238:
2235:
2230:
2221:
2213:
2209:
2202:
2196:
2191:
2181:
2177:
2170:
2166:
2161:
2155:
2149:
2144:
2130:
2122:
2118:
2114:
2111:
2108:
2102:
2096:
2091:
2087:
2083:
2077:
2071:
2068:
2063:
2058:
2052:
2046:
2043:
2031:
2025:
2022:
2019:
2016:
2003:
2002:
2001:
1987:
1958:
1952:
1949:
1946:
1943:
1931:
1929:
1913:
1893:
1873:
1853:
1844:
1831:
1828:
1823:
1819:
1811:
1808:
1796:
1770:
1766:
1758:only through
1739:
1710:
1681:
1673:
1669:
1665:
1662:
1659:
1654:
1650:
1646:
1641:
1637:
1613:
1607:
1601:
1596:
1592:
1588:
1582:
1576:
1573:
1568:
1563:
1557:
1551:
1548:
1542:
1539:
1536:
1523:
1522:
1521:
1498:
1492:
1489:
1486:
1483:
1454:
1449:
1439:
1431:
1428:
1422:
1418:
1412:
1408:
1404:
1401:
1394:
1391:
1372:
1369:
1362:
1359:
1347:
1336:
1335:
1334:
1314:
1291:
1288:
1277:
1246:
1240:
1237:
1234:
1231:
1217:
1213:
1209:
1205:
1204:supersymmetry
1190:
1187:
1177:
1174:
1171:
1168:
1159:
1157:
1141:
1138:
1135:
1132:
1126:
1123:
1117:
1114:
1090:
1087:
1075:
1068:
1063:
1059:
1038:
1035:
1032:
1029:
1026:
1023:
1020:
998:
994:
985:
969:
966:
950:
936:
933:
923:
920:
917:
914:
902:
900:
898:
882:
879:
875:
866:
859:
856:
853:
849:
840:
833:
830:
827:
822:
818:
814:
810:
801:
794:
791:
788:
785:
758:
752:
747:
737:
728:
724:
720:
714:
707:
698:
685:
677:
673:
669:
663:
657:
654:
649:
639:
632:
626:
619:
610:
601:
591:
584:
578:
572:
567:
563:
559:
553:
545:
541:
537:
532:
528:
518:
512:
506:
499:
490:
477:
471:
465:
459:
456:
453:
447:
441:
438:
426:
420:
417:
414:
411:
398:
397:
396:
382:
379:
369:
366:
363:
360:
331:
325:
322:
319:
316:
301:
299:
291:
289:
275:
272:
262:
259:
256:
253:
245:
240:
238:
237:Lorentz group
234:
230:
226:
222:
206:
203:
193:
190:
187:
184:
164:
161:
151:
148:
145:
142:
130:
128:
126:
122:
118:
114:
110:
102:
100:
98:
94:
89:
87:
83:
79:
78:superpartners
75:
70:
68:
64:
60:
56:
51:
49:
45:
41:
37:
33:
19:
4952:Supergravity
4845:Localization
4835:Witten index
4810:Moduli space
4774:
4704:Superalgebra
4671:Supergravity
4585:
4574:
4543:
4539:
4513:
4501:. Retrieved
4481:
4477:
4467:
4435:. Retrieved
4404:
4397:
4352:
4321:
4281:
4277:
4246:
3988:
3984:
3953:
3888:, while for
3719:
3710:Fayet (1976)
3705:
3703:
3697:
3693:
3680:
3676:
3635:
3633:
3611:
3531:superpartner
3508:
3265:
3258:
3091:
2555:
2522:
2510:
2502:
2318:
2313:
2309:
2307:
1932:
1845:
1628:
1469:
1211:
1207:
1160:
951:
906:
777:
302:
295:
243:
241:
134:
125:Bruno Zumino
106:
90:
71:
54:
52:
35:
29:
5092:Researchers
5078:Stop squark
5043:Graviscalar
5038:Graviphoton
4902:WessâZumino
4765:Supercharge
4244:concisely.
4095:gauge group
4012:gauge field
4010:contains a
3227:gauge field
1216:pulled back
897:irreducible
221:gauge boson
121:Julius Wess
109:Abdus Salam
5139:Iliopoulos
5083:Superghost
5073:Sgoldstino
5058:Neutralino
4850:Mu problem
4770:R-symmetry
4734:Superspace
4729:Supergroup
4389:References
3684:, a Dirac
2346:satisfies
984:superspace
59:superspace
55:superfield
18:Superfield
5109:Batchelor
5033:Goldstino
4922:Super QCD
4800:FI D-term
4785:BPS state
4525:1011.1491
4457:ignored (
4447:cite book
4225:ψ
4219:ϕ
4210:Φ
4187:λ
4179:μ
4077:ϕ
4057:ψ
4051:λ
4026:μ
3998:Ψ
3783:⋯
3690:auxiliary
3546:μ
3517:λ
3479:¯
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3463:θ
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2222:θ
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2023:θ
2011:Φ
1962:¯
1959:θ
1950:θ
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1800:¯
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1127:˙
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1033:…
1021:μ
999:μ
870:¯
867:ξ
857:ξ
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802:χ
792:χ
786:ϕ
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725:θ
702:¯
699:ξ
689:¯
686:θ
674:θ
658:ξ
655:θ
643:¯
640:θ
614:¯
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592:θ
564:θ
546:μ
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529:σ
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460:χ
457:θ
442:ϕ
430:¯
427:θ
418:θ
406:Φ
335:¯
332:θ
323:θ
311:Φ
246:, and in
239:changes.
97:operators
74:particles
5204:Category
5144:Montonen
5068:Sfermion
5063:R-hadron
5048:Higgsino
5023:Chargino
4912:4D N = 1
4869:Theorems
4758:Concepts
4367:See also
3560:, while
1906:, named
1304:, where
876:′
850:′
811:′
708:′
620:′
500:′
229:graviton
86:fermions
5159:Seiberg
5134:Golfand
5114:Berezin
5099:Affleck
5028:Gaugino
4568:0416304
4548:Bibcode
4503:3 April
4486:Bibcode
4437:3 April
4410:Bibcode
3674:scalars
3608:Scalars
3529:is the
103:History
63:section
53:Then a
5189:Zumino
5184:Witten
5174:Rogers
5164:Siegel
5104:Bagger
4805:F-term
4795:D-term
4566:
4428:
4383:F-term
4378:D-term
4040:, two
3985:vector
3686:spinor
3602:D-term
2385:where
1928:F-term
1629:where
1156:spinor
778:where
225:spinor
82:bosons
80:where
65:of an
5169:RoÄek
5154:Salam
5149:Olive
5129:Gates
5124:Fayet
5018:Axino
4932:NMSSM
4598:arXiv
4520:arXiv
4318:N = 4
4093:of a
3950:N = 2
3619:torus
3509:Then
1107:with
42:of a
38:is a
5179:Wess
5119:Dine
4927:MSSM
4505:2023
4459:help
4439:2023
4426:ISBN
4322:The
4247:The
3954:The
3292:and
3196:and
3116:and
1206:, a
298:2001
123:and
111:and
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4556:doi
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4494:doi
4418:doi
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353:in
300:).
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