3076:
2634:
3071:{\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).}
761:
2287:
390:
1995:
3493:
756:{\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)}
2282:{\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).}
1454:
2487:
3320:
882:
3601:
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
1613:
1328:
3614:
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.
1687:
1094:
2380:
3488:{\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.}
1831:
1507:
1255:
340:
3792:
2593:
1967:
1141:
1291:
4189:
2372:
1190:
936:
382:
275:
206:
164:
4227:
3210:
4339:
4301:
4264:
4144:
4114:
3971:
3933:
3875:
3821:
3659:
2540:
2333:
1745:
1716:
1038:
969:
3183:
4056:
3903:
3845:
2626:
1320:
50:
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
4773:
4027:
3547:
3516:
3243:
1772:
1000:
231:
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
3279:
4869:
4076:
3997:
1873:
1853:
3308:
3154:
4621:
3733:
4920:
3587:
3567:
3123:
3103:
1987:
1913:
1893:
770:
4905:
4895:
4349:
1449:{\displaystyle {\bar {D}}_{\dot {\alpha }}=-{\bar {\partial }}_{\dot {\alpha }}-i\theta ^{\alpha }\sigma _{\alpha {\dot {\alpha }}}^{\mu }\partial _{\mu }.}
1515:
4874:
1621:
4915:
4418:
4925:
2482:{\displaystyle D_{\alpha }=\partial _{\alpha }+i\sigma _{\alpha {\dot {\alpha }}}^{\mu }{\bar {\theta }}^{\dot {\alpha }}\partial _{\mu }.}
4507:
Krippendorf, Sven; Quevedo, Fernando; Schlotterer, Oliver (5 November 2010). "Cambridge
Lectures on Supersymmetry and Extra Dimensions".
1043:
4614:
5041:
4930:
4654:
4968:
4963:
3611:
4900:
1777:
4607:
3736:
1203:. There exists a projection from the (full) superspace to chiral superspace. So, a function over chiral superspace can be
208:
supersymmetry for example), tensor multiplets and gravity multiplets. The highest component of a vector multiplet is a
4864:
4788:
1462:
1210:
295:
4948:
4833:
4649:
4361:
3742:
3249:
4848:
2548:
885:
277:
SUSY, a vector multiplet (whose highest component is a vector) can sometimes be referred to as a chiral multiplet.
4818:
4230:
1925:
1099:
4702:
3603:
104:
in a 1974 article. Operations on superfields and a partial classification were presented a few months later by
4843:
55:
3701:; this term has been abandoned, but the name "hypermultiplet" for some of its representations is still used.
1260:
4149:
5198:
4953:
4803:
4707:
4079:
2338:
1153:
899:
345:
238:
169:
127:
81:
51:
36:
4890:
4828:
4194:
2501:
4983:
4978:
4732:
4712:
3628:
3188:
1204:
221:
32:
4392:
4314:
4276:
4239:
4119:
4089:
3946:
3908:
3850:
3797:
3634:
2515:
2311:
1721:
1692:
1005:
944:
4768:
4717:
4536:
4474:
4398:
3709:
This section records some commonly used irreducible supermultiplets in extended supersymmetry in the
3161:
101:
28:
4035:
3884:
3826:
2598:
4988:
4973:
4958:
4727:
20:
5097:
4669:
4664:
4586:
4508:
4435:
85:
1296:
888:
supermultiplet, and so different constraints are needed to isolate irreducible representations.
3823:. For supermultiplets representing massless particles, on physical grounds the maximum allowed
4414:
4005:
3525:
3501:
3311:
3221:
1750:
978:
3258:
2492:
An antichiral superfield can be constructed as the complex conjugate of a chiral superfield.
4798:
4697:
4684:
4544:
4482:
4406:
4556:
4061:
3982:
1858:
1838:
5127:
5092:
4813:
4808:
4552:
4447:
3878:
3678:
3284:
3130:
5157:
3712:
4540:
4478:
4402:
3739:
construction in the sense that there is a vacuum vector annihilated by the supercharges
877:{\displaystyle \phi ,\chi ,{\bar {\chi }}',V_{\mu },F,{\bar {F}}',\xi ,{\bar {\xi }}',D}
5147:
5132:
4778:
3572:
3552:
3108:
3088:
1972:
1898:
1878:
105:
4462:
5192:
5172:
5152:
5102:
4737:
4674:
4644:
4630:
4567:
4548:
4486:
1608:{\displaystyle \Phi (y,\theta )=\phi (y)+{\sqrt {2}}\theta \psi (y)+\theta ^{2}F(y),}
1192:
225:
65:. It is a feature of supersymmetric field theories that particles form pairs, called
124:
The most commonly used supermultiplets are vector multiplets, chiral multiplets (in
5177:
5162:
5122:
5112:
5107:
4998:
4940:
4823:
4692:
4659:
4345:
4030:
3674:
3662:
3519:
113:
66:
5167:
5142:
5137:
5087:
5066:
5031:
5026:
4753:
4083:
4000:
3215:
209:
109:
97:
4410:
5071:
5061:
5046:
4838:
4758:
4722:
972:
47:
5117:
5021:
4910:
62:
4578:
5056:
5051:
5036:
5011:
285:
Conventions in this section follow the notes by
Figueroa-O'Farrill (
217:
74:
4585:
Figueroa-O'Farrill, J. M. (2001). "Busstepp
Lectures on Supersymmetry".
2500:
For an action which can be defined from a single chiral superfield, see
1682:{\displaystyle y^{\mu }=x^{\mu }+i\theta \sigma ^{\mu }{\bar {\theta }}}
5016:
4591:
4793:
4783:
4371:
4366:
3590:
1922:
The field can then be expressed in terms of the original coordinates
1916:
1144:
213:
70:
2545:
A vector superfield (also known as a real superfield) is a function
1689:. The superfield is independent of the 'conjugate spin coordinates'
224:, although the organization of the fields as representations of the
3610:
is a vector multiplet containing d real scalars. Similarly, in an
1875:
is a Weyl spinor. There is also the auxiliary complex scalar field
1089:{\displaystyle \theta _{\alpha },{\bar {\theta }}^{\dot {\alpha }}}
5006:
4513:
3693:
The name "hypermultiplet" comes from old term "hypersymmetry" for
3607:
3248:
Their transformation properties and uses are further discussed in
4599:
4603:
4344:
contains one gauge field, four Weyl fermions, six scalars, and
4273:
consists of two Weyl fermions and two complex scalars, or two
3314:. In this gauge, the expansion takes on the much simpler form
80:
These supersymmetric fields are used to build supersymmetric
4320:
4282:
4245:
4125:
4095:
3952:
3914:
3890:
3856:
3832:
3807:
3779:
3640:
2521:
1171:
950:
917:
363:
256:
187:
145:
2301:, which is the complex conjugate of chiral superspace, and
212:, the highest component of a chiral or hypermultiplet is a
3569:
is an auxiliary scalar field. It is conventionally called
1322:
is the covariant derivative, given in index notation as
975:. Superspace contains the usual space-time coordinates
3661:
supersymmetry in 4 dimensions, containing two complex
3043:
2993:
2943:
2859:
2732:
2689:
1826:{\displaystyle {\bar {D}}_{\dot {\alpha }}y^{\mu }=0.}
286:
4461:
Ferrara, Sergio; Wess, Julius; Zumino, Bruno (1974).
4317:
4279:
4242:
4197:
4152:
4122:
4092:
4064:
4038:
4008:
3985:
3949:
3911:
3887:
3853:
3829:
3800:
3745:
3715:
3637:
3606:, while its dimensional reduction on a d-dimensional
3575:
3555:
3528:
3504:
3323:
3287:
3261:
3224:
3191:
3164:
3133:
3111:
3091:
2637:
2601:
2551:
2518:
2383:
2341:
2314:
1998:
1975:
1928:
1901:
1881:
1861:
1841:
1780:
1753:
1724:
1695:
1624:
1518:
1465:
1331:
1299:
1263:
1213:
1156:
1102:
1046:
1008:
981:
947:
902:
773:
393:
348:
298:
241:
220:. The names are defined so as to be invariant under
172:
130:
61:
Phenomenologically, superfields are used to describe
216:, the highest component of a gravity multiplet is a
5080:
4997:
4939:
4883:
4857:
4746:
4683:
4637:
4333:
4295:
4258:
4221:
4183:
4138:
4108:
4070:
4050:
4021:
3991:
3965:
3927:
3897:
3869:
3839:
3815:
3786:
3727:
3653:
3581:
3561:
3541:
3510:
3487:
3302:
3273:
3237:
3204:
3177:
3148:
3117:
3097:
3070:
2620:
2587:
2534:
2481:
2366:
2327:
2281:
1981:
1961:
1907:
1887:
1867:
1847:
1825:
1766:
1739:
1710:
1681:
1607:
1501:
1448:
1314:
1285:
1249:
1184:
1135:
1088:
1032:
994:
963:
930:
896:A (anti-)chiral superfield is a supermultiplet of
876:
755:
376:
334:
269:
200:
158:
1502:{\displaystyle \Phi (x,\theta ,{\bar {\theta }})}
1250:{\displaystyle \Phi (x,\theta ,{\bar {\theta }})}
971:supersymmetry may be written using the notion of
335:{\displaystyle \Phi (x,\theta ,{\bar {\theta }})}
3787:{\displaystyle Q^{A},A=1,\cdots ,{\mathcal {N}}}
1919:which plays an important role in some theories.
166:supersymmetry for example), hypermultiplets (in
4527:Fayet, P. (1976), "Fermi-Bose hypersymmetry",
4086:). These can also be organised into a pair of
4615:
2588:{\displaystyle V(x,\theta ,{\bar {\theta }})}
2512:The vector superfield is a supermultiplet of
884:are different complex fields. This is not an
16:A representation of the supersymmetry algebra
8:
1962:{\displaystyle (x,\theta ,{\bar {\theta }})}
1136:{\displaystyle \alpha ,{\dot {\alpha }}=1,2}
4575:N=2 supersymmetric dynamics for pedestrians
3627:is a type of representation of an extended
4622:
4608:
4600:
1835:The expansion has the interpretation that
4590:
4512:
4319:
4318:
4316:
4281:
4280:
4278:
4244:
4243:
4241:
4229:. Such a multiplet can be used to define
4196:
4166:
4151:
4124:
4123:
4121:
4094:
4093:
4091:
4063:
4037:
4013:
4007:
3984:
3951:
3950:
3948:
3913:
3912:
3910:
3889:
3888:
3886:
3855:
3854:
3852:
3831:
3830:
3828:
3806:
3805:
3799:
3778:
3777:
3750:
3744:
3714:
3639:
3638:
3636:
3574:
3554:
3533:
3527:
3503:
3473:
3462:
3461:
3454:
3440:
3425:
3414:
3413:
3398:
3397:
3386:
3385:
3379:
3366:
3351:
3350:
3344:
3328:
3322:
3286:
3260:
3229:
3223:
3196:
3190:
3169:
3163:
3132:
3110:
3090:
3042:
3025:
3015:
3008:
2992:
2974:
2968:
2958:
2942:
2922:
2912:
2891:
2881:
2871:
2858:
2845:
2830:
2824:
2808:
2794:
2788:
2749:
2743:
2731:
2704:
2688:
2675:
2665:
2636:
2612:
2600:
2571:
2570:
2550:
2520:
2519:
2517:
2470:
2454:
2453:
2442:
2441:
2434:
2422:
2421:
2417:
2401:
2388:
2382:
2349:
2340:
2319:
2313:
2255:
2244:
2243:
2236:
2222:
2208:
2207:
2201:
2179:
2169:
2153:
2132:
2117:
2116:
2110:
2079:
2050:
2018:
2017:
1997:
1974:
1945:
1944:
1927:
1900:
1880:
1860:
1840:
1811:
1795:
1794:
1783:
1782:
1779:
1758:
1752:
1726:
1725:
1723:
1697:
1696:
1694:
1668:
1667:
1661:
1642:
1629:
1623:
1584:
1555:
1517:
1485:
1484:
1464:
1437:
1427:
1415:
1414:
1410:
1400:
1378:
1377:
1366:
1365:
1346:
1345:
1334:
1333:
1330:
1301:
1300:
1298:
1264:
1262:
1233:
1232:
1212:
1170:
1169:
1155:
1143:, transforming as a two-component (Weyl)
1110:
1109:
1101:
1074:
1073:
1062:
1061:
1051:
1045:
1007:
986:
980:
949:
948:
946:
916:
915:
901:
853:
852:
827:
826:
810:
788:
787:
772:
735:
724:
723:
716:
685:
684:
672:
671:
665:
637:
626:
625:
597:
596:
589:
578:
577:
555:
533:
520:
505:
504:
477:
476:
464:
463:
413:
412:
392:
362:
361:
347:
318:
317:
297:
281:Superfields in d = 4, N = 1 supersymmetry
255:
254:
240:
186:
185:
171:
144:
143:
129:
4391:Salam, Abdus; Strathdee, J. (May 1994).
3631:, in particular the matter multiplet of
3255:Using gauge transformations, the fields
1207:to the full superspace. Such a function
4463:"Supergauge multiplets and superfields"
4383:
1040:, and four extra fermionic coordinates
4443:
4433:
4350:N = 4 supersymmetric YangâMills theory
2595:which satisfies the reality condition
1286:{\displaystyle {\overline {D}}\Phi =0}
4184:{\displaystyle W=(A_{\mu },\lambda )}
3698:
3310:can be set to zero. This is known as
7:
2628:. Such a field admits the expansion
2367:{\displaystyle D\Phi ^{\dagger }=0,}
1185:{\displaystyle d=4,{\mathcal {N}}=1}
931:{\displaystyle d=4,{\mathcal {N}}=1}
377:{\displaystyle d=4,{\mathcal {N}}=1}
270:{\displaystyle d=4,{\mathcal {N}}=2}
201:{\displaystyle d=4,{\mathcal {N}}=2}
159:{\displaystyle d=4,{\mathcal {N}}=1}
4222:{\displaystyle \Phi =(\phi ,\psi )}
1969:by substituting the expression for
1257:satisfies the covariant constraint
84:, where the fields are promoted to
4198:
3986:
3205:{\displaystyle \lambda ^{\alpha }}
2965:
2888:
2467:
2398:
2346:
2316:
2176:
2129:
1999:
1519:
1466:
1434:
1368:
1274:
1214:
394:
299:
14:
4397:. Vol. 5. pp. 404â409.
3735:case. These are constructed by a
3705:Extended supersymmetry (N > 1)
384:supersymmetry can be expanded as
4655:Supersymmetric quantum mechanics
4334:{\displaystyle {\mathcal {N}}=4}
4296:{\displaystyle {\mathcal {N}}=1}
4259:{\displaystyle {\mathcal {N}}=2}
4139:{\displaystyle {\mathcal {N}}=1}
4109:{\displaystyle {\mathcal {N}}=1}
3966:{\displaystyle {\mathcal {N}}=2}
3928:{\displaystyle {\mathcal {N}}=4}
3870:{\displaystyle {\mathcal {N}}=8}
3816:{\displaystyle 2^{\mathcal {N}}}
3654:{\displaystyle {\mathcal {N}}=2}
2535:{\displaystyle {\mathcal {N}}=1}
2328:{\displaystyle \Phi ^{\dagger }}
1740:{\displaystyle {\bar {\theta }}}
1718:in the sense that it depends on
1711:{\displaystyle {\bar {\theta }}}
1033:{\displaystyle \mu =0,\ldots ,3}
964:{\displaystyle {\mathcal {N}}=1}
941:In four dimensions, the minimal
56:associated supermultiplet bundle
3178:{\displaystyle \chi _{\alpha }}
2496:Actions from chiral superfields
96:Superfields were introduced by
4216:
4204:
4178:
4159:
4051:{\displaystyle \lambda ,\psi }
3898:{\displaystyle {\mathcal {N}}}
3840:{\displaystyle {\mathcal {N}}}
3467:
3419:
3403:
3391:
3356:
2775:
2760:
2725:
2710:
2621:{\displaystyle V=V^{\dagger }}
2582:
2576:
2555:
2447:
2273:
2267:
2249:
2213:
2194:
2188:
2147:
2141:
2122:
2094:
2088:
2069:
2063:
2044:
2038:
2029:
2023:
2002:
1956:
1950:
1929:
1788:
1731:
1702:
1673:
1599:
1593:
1574:
1568:
1549:
1543:
1534:
1522:
1496:
1490:
1469:
1371:
1339:
1306:
1244:
1238:
1217:
1067:
858:
832:
793:
750:
744:
729:
706:
700:
690:
677:
655:
649:
631:
618:
612:
602:
583:
570:
564:
545:
539:
510:
498:
492:
482:
469:
457:
451:
439:
433:
424:
418:
397:
329:
323:
302:
1:
4078:(which also transform in the
3737:highest-weight representation
292:A general complex superfield
4549:10.1016/0550-3213(76)90458-2
4487:10.1016/0370-2693(74)90283-4
4348:conjugates. This appears in
3794:. The irreps have dimension
3020:
2979:
2917:
2876:
2850:
2835:
2799:
2755:
2680:
2670:
1269:
4650:Supersymmetric gauge theory
4394:Super-Gauge Transformations
4362:Supersymmetric gauge theory
3250:supersymmetric gauge theory
3081:The constituent fields are
1915:by convention: this is the
1855:is a complex scalar field,
5215:
4949:Pure 4D N = 1 supergravity
4411:10.1142/9789812795915_0047
1315:{\displaystyle {\bar {D}}}
4849:Electricâmagnetic duality
3697:=2 supersymmetry used by
2308:An antichiral superfield
2297:Similarly, there is also
1774:. It can be checked that
120:Naming and classification
4870:HaagâĆopuszaĆskiâSohnius
4844:Little hierarchy problem
4022:{\displaystyle A_{\mu }}
3542:{\displaystyle A_{\mu }}
3511:{\displaystyle \lambda }
3238:{\displaystyle A_{\mu }}
1767:{\displaystyle y^{\mu }}
1509:can then be expanded as
995:{\displaystyle x^{\mu }}
4926:6D (2,0) superconformal
3274:{\displaystyle C,\chi }
3158:Two Weyl spinor fields
3127:A complex scalar field
3085:Two real scalar fields
4906:N = 4 super YangâMills
4896:N = 1 super YangâMills
4804:Supersymmetry breaking
4708:Superconformal algebra
4703:Super-Poincaré algebra
4564:A Supersymmetry Primer
4335:
4297:
4260:
4223:
4185:
4140:
4110:
4080:adjoint representation
4072:
4052:
4023:
3993:
3967:
3929:
3899:
3881:, the maximum allowed
3871:
3841:
3817:
3788:
3729:
3655:
3589:, and is known as the
3583:
3563:
3543:
3512:
3489:
3304:
3275:
3239:
3206:
3179:
3150:
3119:
3099:
3072:
2622:
2589:
2536:
2483:
2368:
2329:
2303:antichiral superfields
2293:Antichiral superfields
2283:
1983:
1963:
1909:
1889:
1869:
1849:
1827:
1768:
1741:
1712:
1683:
1609:
1503:
1450:
1316:
1287:
1251:
1186:
1137:
1090:
1034:
996:
965:
932:
878:
757:
378:
336:
271:
202:
160:
82:quantum field theories
37:extended supersymmetry
4984:Type IIB supergravity
4979:Type IIA supergravity
4954:4D N = 1 supergravity
4819:SeibergâWitten theory
4733:Super Minkowski space
4713:Supersymmetry algebra
4336:
4298:
4261:
4231:SeibergâWitten theory
4224:
4191:and chiral multiplet
4186:
4141:
4111:
4073:
4071:{\displaystyle \phi }
4053:
4024:
3994:
3992:{\displaystyle \Psi }
3968:
3930:
3900:
3872:
3842:
3818:
3789:
3730:
3656:
3629:supersymmetry algebra
3612:11-dimensional theory
3584:
3564:
3544:
3513:
3490:
3305:
3276:
3240:
3214:A real vector field (
3207:
3180:
3151:
3120:
3100:
3073:
2623:
2590:
2537:
2484:
2369:
2330:
2299:antichiral superspace
2284:
1984:
1964:
1910:
1890:
1870:
1868:{\displaystyle \psi }
1850:
1848:{\displaystyle \phi }
1828:
1769:
1742:
1713:
1684:
1610:
1504:
1451:
1317:
1288:
1252:
1187:
1138:
1091:
1035:
997:
966:
933:
879:
758:
379:
337:
272:
222:dimensional reduction
203:
161:
33:supersymmetry algebra
4769:Short supermultiplet
4568:arXiv:hep-ph/9709356
4315:
4277:
4240:
4195:
4150:
4120:
4090:
4062:
4036:
4006:
3983:
3947:
3909:
3885:
3851:
3827:
3798:
3743:
3713:
3635:
3604:MajoranaâWeyl spinor
3573:
3553:
3526:
3502:
3321:
3303:{\displaystyle M+iN}
3285:
3259:
3222:
3189:
3162:
3149:{\displaystyle M+iN}
3131:
3109:
3089:
2635:
2599:
2549:
2516:
2381:
2339:
2312:
1996:
1973:
1926:
1899:
1879:
1859:
1839:
1778:
1751:
1722:
1693:
1622:
1516:
1463:
1459:A chiral superfield
1329:
1297:
1261:
1211:
1154:
1100:
1044:
1006:
979:
945:
900:
771:
391:
346:
296:
239:
170:
128:
4989:Gauged supergravity
4974:Type I supergravity
4931:ABJM superconformal
4728:Harmonic superspace
4562:Stephen P. Martin.
4541:1976NuPhB.113..135F
4479:1974PhLB...51..239F
4403:1994spas.book..404S
4303:chiral multiplets.
3728:{\displaystyle d=4}
3677:Ï, and two further
2439:
1432:
1199:is a function over
1147:and its conjugate.
21:theoretical physics
4964:Higher dimensional
4959:N = 8 supergravity
4875:Nonrenormalization
4670:Super vector space
4665:Superstring theory
4331:
4293:
4256:
4219:
4181:
4136:
4106:
4068:
4048:
4019:
3989:
3963:
3925:
3895:
3867:
3837:
3813:
3784:
3725:
3651:
3579:
3559:
3539:
3508:
3485:
3300:
3271:
3235:
3202:
3175:
3146:
3115:
3095:
3068:
3052:
3002:
2952:
2868:
2741:
2698:
2618:
2585:
2532:
2479:
2413:
2364:
2325:
2279:
1979:
1959:
1905:
1885:
1865:
1845:
1823:
1764:
1737:
1708:
1679:
1605:
1499:
1446:
1406:
1312:
1283:
1247:
1182:
1133:
1086:
1030:
992:
961:
928:
874:
753:
374:
332:
267:
198:
156:
5186:
5185:
4829:WessâZumino gauge
4529:Nuclear Physics B
4420:978-981-02-1662-7
4146:vector multiplet
3879:renormalizability
3582:{\displaystyle D}
3562:{\displaystyle D}
3470:
3448:
3422:
3406:
3394:
3359:
3331:
3312:Wess-Zumino gauge
3118:{\displaystyle D}
3098:{\displaystyle C}
3051:
3023:
3001:
2982:
2951:
2920:
2879:
2867:
2853:
2838:
2802:
2758:
2740:
2697:
2683:
2673:
2579:
2508:Vector superfield
2502:WessâZumino model
2462:
2450:
2430:
2252:
2230:
2216:
2163:
2162:
2125:
2055:
2026:
1982:{\displaystyle y}
1953:
1908:{\displaystyle F}
1888:{\displaystyle F}
1803:
1791:
1734:
1705:
1676:
1560:
1493:
1423:
1386:
1374:
1354:
1342:
1309:
1272:
1241:
1201:chiral superspace
1197:chiral superfield
1118:
1082:
1070:
892:Chiral superfield
861:
835:
796:
732:
693:
680:
634:
605:
586:
513:
485:
472:
421:
326:
5206:
4969:11D supergravity
4698:Lie superalgebra
4685:Supermathematics
4624:
4617:
4610:
4601:
4596:
4594:
4573:Yuji Tachikawa.
4559:
4519:
4518:
4516:
4504:
4498:
4497:
4495:
4493:
4458:
4452:
4451:
4445:
4441:
4439:
4431:
4429:
4427:
4388:
4342:vector multiplet
4340:
4338:
4337:
4332:
4324:
4323:
4302:
4300:
4299:
4294:
4286:
4285:
4271:scalar multiplet
4265:
4263:
4262:
4257:
4249:
4248:
4228:
4226:
4225:
4220:
4190:
4188:
4187:
4182:
4171:
4170:
4145:
4143:
4142:
4137:
4129:
4128:
4115:
4113:
4112:
4107:
4099:
4098:
4077:
4075:
4074:
4069:
4057:
4055:
4054:
4049:
4028:
4026:
4025:
4020:
4018:
4017:
3998:
3996:
3995:
3990:
3978:chiral multiplet
3972:
3970:
3969:
3964:
3956:
3955:
3934:
3932:
3931:
3926:
3918:
3917:
3904:
3902:
3901:
3896:
3894:
3893:
3876:
3874:
3873:
3868:
3860:
3859:
3846:
3844:
3843:
3838:
3836:
3835:
3822:
3820:
3819:
3814:
3812:
3811:
3810:
3793:
3791:
3790:
3785:
3783:
3782:
3755:
3754:
3734:
3732:
3731:
3726:
3681:complex scalars
3660:
3658:
3657:
3652:
3644:
3643:
3588:
3586:
3585:
3580:
3568:
3566:
3565:
3560:
3548:
3546:
3545:
3540:
3538:
3537:
3517:
3515:
3514:
3509:
3494:
3492:
3491:
3486:
3478:
3477:
3472:
3471:
3463:
3459:
3458:
3449:
3441:
3430:
3429:
3424:
3423:
3415:
3408:
3407:
3399:
3396:
3395:
3387:
3384:
3383:
3371:
3370:
3361:
3360:
3352:
3349:
3348:
3333:
3332:
3329:
3309:
3307:
3306:
3301:
3280:
3278:
3277:
3272:
3244:
3242:
3241:
3236:
3234:
3233:
3211:
3209:
3208:
3203:
3201:
3200:
3184:
3182:
3181:
3176:
3174:
3173:
3155:
3153:
3152:
3147:
3124:
3122:
3121:
3116:
3104:
3102:
3101:
3096:
3077:
3075:
3074:
3069:
3064:
3060:
3053:
3044:
3030:
3029:
3024:
3016:
3013:
3012:
3003:
2994:
2988:
2984:
2983:
2975:
2973:
2972:
2963:
2962:
2953:
2944:
2927:
2926:
2921:
2913:
2904:
2900:
2896:
2895:
2886:
2885:
2880:
2872:
2869:
2860:
2854:
2846:
2839:
2831:
2829:
2828:
2813:
2812:
2803:
2795:
2793:
2792:
2759:
2754:
2753:
2744:
2742:
2733:
2709:
2708:
2699:
2690:
2684:
2676:
2674:
2666:
2627:
2625:
2624:
2619:
2617:
2616:
2594:
2592:
2591:
2586:
2581:
2580:
2572:
2541:
2539:
2538:
2533:
2525:
2524:
2488:
2486:
2485:
2480:
2475:
2474:
2465:
2464:
2463:
2455:
2452:
2451:
2443:
2438:
2433:
2432:
2431:
2423:
2406:
2405:
2393:
2392:
2373:
2371:
2370:
2365:
2354:
2353:
2334:
2332:
2331:
2326:
2324:
2323:
2288:
2286:
2285:
2280:
2260:
2259:
2254:
2253:
2245:
2241:
2240:
2231:
2223:
2218:
2217:
2209:
2206:
2205:
2184:
2183:
2174:
2173:
2164:
2158:
2154:
2137:
2136:
2127:
2126:
2118:
2115:
2114:
2084:
2083:
2056:
2051:
2028:
2027:
2019:
1988:
1986:
1985:
1980:
1968:
1966:
1965:
1960:
1955:
1954:
1946:
1914:
1912:
1911:
1906:
1894:
1892:
1891:
1886:
1874:
1872:
1871:
1866:
1854:
1852:
1851:
1846:
1832:
1830:
1829:
1824:
1816:
1815:
1806:
1805:
1804:
1796:
1793:
1792:
1784:
1773:
1771:
1770:
1765:
1763:
1762:
1746:
1744:
1743:
1738:
1736:
1735:
1727:
1717:
1715:
1714:
1709:
1707:
1706:
1698:
1688:
1686:
1685:
1680:
1678:
1677:
1669:
1666:
1665:
1647:
1646:
1634:
1633:
1614:
1612:
1611:
1606:
1589:
1588:
1561:
1556:
1508:
1506:
1505:
1500:
1495:
1494:
1486:
1455:
1453:
1452:
1447:
1442:
1441:
1431:
1426:
1425:
1424:
1416:
1405:
1404:
1389:
1388:
1387:
1379:
1376:
1375:
1367:
1357:
1356:
1355:
1347:
1344:
1343:
1335:
1321:
1319:
1318:
1313:
1311:
1310:
1302:
1292:
1290:
1289:
1284:
1273:
1265:
1256:
1254:
1253:
1248:
1243:
1242:
1234:
1191:
1189:
1188:
1183:
1175:
1174:
1142:
1140:
1139:
1134:
1120:
1119:
1111:
1095:
1093:
1092:
1087:
1085:
1084:
1083:
1075:
1072:
1071:
1063:
1056:
1055:
1039:
1037:
1036:
1031:
1001:
999:
998:
993:
991:
990:
970:
968:
967:
962:
954:
953:
937:
935:
934:
929:
921:
920:
883:
881:
880:
875:
867:
863:
862:
854:
841:
837:
836:
828:
815:
814:
802:
798:
797:
789:
762:
760:
759:
754:
740:
739:
734:
733:
725:
721:
720:
699:
695:
694:
686:
682:
681:
673:
670:
669:
642:
641:
636:
635:
627:
611:
607:
606:
598:
594:
593:
588:
587:
579:
560:
559:
538:
537:
525:
524:
515:
514:
506:
491:
487:
486:
478:
474:
473:
465:
423:
422:
414:
383:
381:
380:
375:
367:
366:
341:
339:
338:
333:
328:
327:
319:
276:
274:
273:
268:
260:
259:
233:scalar multiplet
207:
205:
204:
199:
191:
190:
165:
163:
162:
157:
149:
148:
73:are paired with
35:, possibly with
5214:
5213:
5209:
5208:
5207:
5205:
5204:
5203:
5189:
5188:
5187:
5182:
5076:
4993:
4935:
4879:
4865:ColemanâMandula
4853:
4814:Seiberg duality
4809:Konishi anomaly
4742:
4679:
4633:
4628:
4584:
4579:arXiv:1312.2684
4526:
4523:
4522:
4506:
4505:
4501:
4491:
4489:
4460:
4459:
4455:
4442:
4432:
4425:
4423:
4421:
4390:
4389:
4385:
4380:
4358:
4313:
4312:
4309:
4275:
4274:
4238:
4237:
4193:
4192:
4162:
4148:
4147:
4118:
4117:
4116:multiplets, an
4088:
4087:
4060:
4059:
4058:, and a scalar
4034:
4033:
4009:
4004:
4003:
3981:
3980:
3945:
3944:
3941:
3907:
3906:
3883:
3882:
3849:
3848:
3825:
3824:
3801:
3796:
3795:
3746:
3741:
3740:
3711:
3710:
3707:
3689:
3672:
3633:
3632:
3621:
3599:
3571:
3570:
3551:
3550:
3529:
3524:
3523:
3500:
3499:
3460:
3450:
3412:
3375:
3362:
3340:
3324:
3319:
3318:
3283:
3282:
3257:
3256:
3225:
3220:
3219:
3192:
3187:
3186:
3165:
3160:
3159:
3129:
3128:
3107:
3106:
3087:
3086:
3035:
3031:
3014:
3004:
2964:
2954:
2935:
2931:
2911:
2887:
2870:
2844:
2840:
2820:
2804:
2784:
2745:
2700:
2633:
2632:
2608:
2597:
2596:
2547:
2546:
2542:supersymmetry.
2514:
2513:
2510:
2498:
2466:
2440:
2397:
2384:
2379:
2378:
2345:
2337:
2336:
2315:
2310:
2309:
2295:
2242:
2232:
2197:
2175:
2165:
2128:
2106:
2075:
1994:
1993:
1971:
1970:
1924:
1923:
1897:
1896:
1877:
1876:
1857:
1856:
1837:
1836:
1807:
1781:
1776:
1775:
1754:
1749:
1748:
1720:
1719:
1691:
1690:
1657:
1638:
1625:
1620:
1619:
1580:
1514:
1513:
1461:
1460:
1433:
1396:
1364:
1332:
1327:
1326:
1295:
1294:
1259:
1258:
1209:
1208:
1152:
1151:
1098:
1097:
1060:
1047:
1042:
1041:
1004:
1003:
982:
977:
976:
943:
942:
938:supersymmetry.
898:
897:
894:
851:
825:
806:
786:
769:
768:
722:
712:
683:
661:
624:
595:
576:
551:
529:
516:
475:
389:
388:
344:
343:
294:
293:
283:
237:
236:
168:
167:
126:
125:
122:
102:J. A. Strathdee
94:
17:
12:
11:
5:
5212:
5210:
5202:
5201:
5191:
5190:
5184:
5183:
5181:
5180:
5175:
5170:
5165:
5160:
5155:
5150:
5145:
5140:
5135:
5130:
5125:
5120:
5115:
5110:
5105:
5100:
5095:
5090:
5084:
5082:
5078:
5077:
5075:
5074:
5069:
5064:
5059:
5054:
5049:
5044:
5039:
5034:
5029:
5024:
5019:
5014:
5009:
5003:
5001:
4995:
4994:
4992:
4991:
4986:
4981:
4976:
4971:
4966:
4961:
4956:
4951:
4945:
4943:
4937:
4936:
4934:
4933:
4928:
4923:
4918:
4913:
4908:
4903:
4898:
4893:
4887:
4885:
4884:Field theories
4881:
4880:
4878:
4877:
4872:
4867:
4861:
4859:
4855:
4854:
4852:
4851:
4846:
4841:
4836:
4831:
4826:
4821:
4816:
4811:
4806:
4801:
4796:
4791:
4786:
4781:
4779:Superpotential
4776:
4771:
4766:
4764:Supermultiplet
4761:
4756:
4750:
4748:
4744:
4743:
4741:
4740:
4735:
4730:
4725:
4720:
4715:
4710:
4705:
4700:
4695:
4689:
4687:
4681:
4680:
4678:
4677:
4672:
4667:
4662:
4657:
4652:
4647:
4641:
4639:
4638:General topics
4635:
4634:
4629:
4627:
4626:
4619:
4612:
4604:
4598:
4597:
4592:hep-th/0109172
4582:
4571:
4560:
4535:(1): 135â155,
4521:
4520:
4499:
4473:(3): 239â241.
4453:
4444:|journal=
4419:
4382:
4381:
4379:
4376:
4375:
4374:
4369:
4364:
4357:
4354:
4330:
4327:
4322:
4308:
4305:
4292:
4289:
4284:
4267:hypermultiplet
4255:
4252:
4247:
4218:
4215:
4212:
4209:
4206:
4203:
4200:
4180:
4177:
4174:
4169:
4165:
4161:
4158:
4155:
4135:
4132:
4127:
4105:
4102:
4097:
4067:
4047:
4044:
4041:
4016:
4012:
3988:
3962:
3959:
3954:
3940:
3937:
3924:
3921:
3916:
3892:
3866:
3863:
3858:
3834:
3809:
3804:
3781:
3776:
3773:
3770:
3767:
3764:
3761:
3758:
3753:
3749:
3724:
3721:
3718:
3706:
3703:
3685:
3668:
3650:
3647:
3642:
3625:hypermultiplet
3620:
3619:Hypermultiplet
3617:
3598:
3595:
3578:
3558:
3536:
3532:
3507:
3496:
3495:
3484:
3481:
3476:
3469:
3466:
3457:
3453:
3447:
3444:
3439:
3436:
3433:
3428:
3421:
3418:
3411:
3405:
3402:
3393:
3390:
3382:
3378:
3374:
3369:
3365:
3358:
3355:
3347:
3343:
3339:
3336:
3327:
3299:
3296:
3293:
3290:
3270:
3267:
3264:
3246:
3245:
3232:
3228:
3212:
3199:
3195:
3172:
3168:
3156:
3145:
3142:
3139:
3136:
3125:
3114:
3094:
3079:
3078:
3067:
3063:
3059:
3056:
3050:
3047:
3041:
3038:
3034:
3028:
3022:
3019:
3011:
3007:
3000:
2997:
2991:
2987:
2981:
2978:
2971:
2967:
2961:
2957:
2950:
2947:
2941:
2938:
2934:
2930:
2925:
2919:
2916:
2910:
2907:
2903:
2899:
2894:
2890:
2884:
2878:
2875:
2866:
2863:
2857:
2852:
2849:
2843:
2837:
2834:
2827:
2823:
2819:
2816:
2811:
2807:
2801:
2798:
2791:
2787:
2783:
2780:
2777:
2774:
2771:
2768:
2765:
2762:
2757:
2752:
2748:
2739:
2736:
2730:
2727:
2724:
2721:
2718:
2715:
2712:
2707:
2703:
2696:
2693:
2687:
2682:
2679:
2672:
2669:
2664:
2661:
2658:
2655:
2652:
2649:
2646:
2643:
2640:
2615:
2611:
2607:
2604:
2584:
2578:
2575:
2569:
2566:
2563:
2560:
2557:
2554:
2531:
2528:
2523:
2509:
2506:
2497:
2494:
2490:
2489:
2478:
2473:
2469:
2461:
2458:
2449:
2446:
2437:
2429:
2426:
2420:
2416:
2412:
2409:
2404:
2400:
2396:
2391:
2387:
2363:
2360:
2357:
2352:
2348:
2344:
2322:
2318:
2294:
2291:
2290:
2289:
2278:
2275:
2272:
2269:
2266:
2263:
2258:
2251:
2248:
2239:
2235:
2229:
2226:
2221:
2215:
2212:
2204:
2200:
2196:
2193:
2190:
2187:
2182:
2178:
2172:
2168:
2161:
2157:
2152:
2149:
2146:
2143:
2140:
2135:
2131:
2124:
2121:
2113:
2109:
2105:
2102:
2099:
2096:
2093:
2090:
2087:
2082:
2078:
2074:
2071:
2068:
2065:
2062:
2059:
2054:
2049:
2046:
2043:
2040:
2037:
2034:
2031:
2025:
2022:
2016:
2013:
2010:
2007:
2004:
2001:
1978:
1958:
1952:
1949:
1943:
1940:
1937:
1934:
1931:
1904:
1884:
1864:
1844:
1822:
1819:
1814:
1810:
1802:
1799:
1790:
1787:
1761:
1757:
1733:
1730:
1704:
1701:
1675:
1672:
1664:
1660:
1656:
1653:
1650:
1645:
1641:
1637:
1632:
1628:
1616:
1615:
1604:
1601:
1598:
1595:
1592:
1587:
1583:
1579:
1576:
1573:
1570:
1567:
1564:
1559:
1554:
1551:
1548:
1545:
1542:
1539:
1536:
1533:
1530:
1527:
1524:
1521:
1498:
1492:
1489:
1483:
1480:
1477:
1474:
1471:
1468:
1457:
1456:
1445:
1440:
1436:
1430:
1422:
1419:
1413:
1409:
1403:
1399:
1395:
1392:
1385:
1382:
1373:
1370:
1363:
1360:
1353:
1350:
1341:
1338:
1308:
1305:
1282:
1279:
1276:
1271:
1268:
1246:
1240:
1237:
1231:
1228:
1225:
1222:
1219:
1216:
1181:
1178:
1173:
1168:
1165:
1162:
1159:
1132:
1129:
1126:
1123:
1117:
1114:
1108:
1105:
1081:
1078:
1069:
1066:
1059:
1054:
1050:
1029:
1026:
1023:
1020:
1017:
1014:
1011:
989:
985:
960:
957:
952:
927:
924:
919:
914:
911:
908:
905:
893:
890:
873:
870:
866:
860:
857:
850:
847:
844:
840:
834:
831:
824:
821:
818:
813:
809:
805:
801:
795:
792:
785:
782:
779:
776:
765:
764:
752:
749:
746:
743:
738:
731:
728:
719:
715:
711:
708:
705:
702:
698:
692:
689:
679:
676:
668:
664:
660:
657:
654:
651:
648:
645:
640:
633:
630:
623:
620:
617:
614:
610:
604:
601:
592:
585:
582:
575:
572:
569:
566:
563:
558:
554:
550:
547:
544:
541:
536:
532:
528:
523:
519:
512:
509:
503:
500:
497:
494:
490:
484:
481:
471:
468:
462:
459:
456:
453:
450:
447:
444:
441:
438:
435:
432:
429:
426:
420:
417:
411:
408:
405:
402:
399:
396:
373:
370:
365:
360:
357:
354:
351:
331:
325:
322:
316:
313:
310:
307:
304:
301:
282:
279:
266:
263:
258:
253:
250:
247:
244:
197:
194:
189:
184:
181:
178:
175:
155:
152:
147:
142:
139:
136:
133:
121:
118:
106:Sergio Ferrara
93:
90:
46:is a field on
29:representation
25:supermultiplet
15:
13:
10:
9:
6:
4:
3:
2:
5211:
5200:
5199:Supersymmetry
5197:
5196:
5194:
5179:
5176:
5174:
5171:
5169:
5166:
5164:
5161:
5159:
5156:
5154:
5151:
5149:
5146:
5144:
5141:
5139:
5136:
5134:
5131:
5129:
5126:
5124:
5121:
5119:
5116:
5114:
5111:
5109:
5106:
5104:
5101:
5099:
5096:
5094:
5091:
5089:
5086:
5085:
5083:
5079:
5073:
5070:
5068:
5065:
5063:
5060:
5058:
5055:
5053:
5050:
5048:
5045:
5043:
5040:
5038:
5035:
5033:
5030:
5028:
5025:
5023:
5020:
5018:
5015:
5013:
5010:
5008:
5005:
5004:
5002:
5000:
4999:Superpartners
4996:
4990:
4987:
4985:
4982:
4980:
4977:
4975:
4972:
4970:
4967:
4965:
4962:
4960:
4957:
4955:
4952:
4950:
4947:
4946:
4944:
4942:
4938:
4932:
4929:
4927:
4924:
4922:
4919:
4917:
4914:
4912:
4909:
4907:
4904:
4902:
4899:
4897:
4894:
4892:
4889:
4888:
4886:
4882:
4876:
4873:
4871:
4868:
4866:
4863:
4862:
4860:
4856:
4850:
4847:
4845:
4842:
4840:
4837:
4835:
4832:
4830:
4827:
4825:
4822:
4820:
4817:
4815:
4812:
4810:
4807:
4805:
4802:
4800:
4797:
4795:
4792:
4790:
4787:
4785:
4782:
4780:
4777:
4775:
4772:
4770:
4767:
4765:
4762:
4760:
4757:
4755:
4752:
4751:
4749:
4745:
4739:
4738:Supermanifold
4736:
4734:
4731:
4729:
4726:
4724:
4721:
4719:
4716:
4714:
4711:
4709:
4706:
4704:
4701:
4699:
4696:
4694:
4691:
4690:
4688:
4686:
4682:
4676:
4675:Supergeometry
4673:
4671:
4668:
4666:
4663:
4661:
4658:
4656:
4653:
4651:
4648:
4646:
4645:Supersymmetry
4643:
4642:
4640:
4636:
4632:
4631:Supersymmetry
4625:
4620:
4618:
4613:
4611:
4606:
4605:
4602:
4593:
4588:
4583:
4580:
4576:
4572:
4569:
4565:
4561:
4558:
4554:
4550:
4546:
4542:
4538:
4534:
4530:
4525:
4524:
4515:
4510:
4503:
4500:
4488:
4484:
4480:
4476:
4472:
4468:
4467:Phys. Lett. B
4464:
4457:
4454:
4449:
4437:
4422:
4416:
4412:
4408:
4404:
4400:
4396:
4395:
4387:
4384:
4377:
4373:
4370:
4368:
4365:
4363:
4360:
4359:
4355:
4353:
4351:
4347:
4343:
4328:
4325:
4306:
4304:
4290:
4287:
4272:
4268:
4253:
4250:
4234:
4232:
4213:
4210:
4207:
4201:
4175:
4172:
4167:
4163:
4156:
4153:
4133:
4130:
4103:
4100:
4085:
4081:
4065:
4045:
4042:
4039:
4032:
4031:Weyl fermions
4014:
4010:
4002:
3979:
3975:
3960:
3957:
3938:
3936:
3922:
3919:
3880:
3864:
3861:
3802:
3774:
3771:
3768:
3765:
3762:
3759:
3756:
3751:
3747:
3738:
3722:
3719:
3716:
3704:
3702:
3700:
3696:
3691:
3688:
3684:
3680:
3676:
3671:
3667:
3664:
3648:
3645:
3630:
3626:
3618:
3616:
3613:
3609:
3605:
3596:
3594:
3592:
3576:
3556:
3534:
3530:
3521:
3505:
3482:
3479:
3474:
3464:
3455:
3451:
3445:
3442:
3437:
3434:
3431:
3426:
3416:
3409:
3400:
3388:
3380:
3376:
3372:
3367:
3363:
3353:
3345:
3341:
3337:
3334:
3325:
3317:
3316:
3315:
3313:
3297:
3294:
3291:
3288:
3268:
3265:
3262:
3253:
3251:
3230:
3226:
3217:
3213:
3197:
3193:
3170:
3166:
3157:
3143:
3140:
3137:
3134:
3126:
3112:
3092:
3084:
3083:
3082:
3065:
3061:
3057:
3054:
3048:
3045:
3039:
3036:
3032:
3026:
3017:
3009:
3005:
2998:
2995:
2989:
2985:
2976:
2969:
2959:
2955:
2948:
2945:
2939:
2936:
2932:
2928:
2923:
2914:
2908:
2905:
2901:
2897:
2892:
2882:
2873:
2864:
2861:
2855:
2847:
2841:
2832:
2825:
2821:
2817:
2814:
2809:
2805:
2796:
2789:
2785:
2781:
2778:
2772:
2769:
2766:
2763:
2750:
2746:
2737:
2734:
2728:
2722:
2719:
2716:
2713:
2705:
2701:
2694:
2691:
2685:
2677:
2667:
2662:
2659:
2656:
2653:
2650:
2647:
2644:
2641:
2638:
2631:
2630:
2629:
2613:
2609:
2605:
2602:
2573:
2567:
2564:
2561:
2558:
2552:
2543:
2529:
2526:
2507:
2505:
2503:
2495:
2493:
2476:
2471:
2459:
2456:
2444:
2435:
2427:
2424:
2418:
2414:
2410:
2407:
2402:
2394:
2389:
2385:
2377:
2376:
2375:
2361:
2358:
2355:
2350:
2342:
2320:
2306:
2304:
2300:
2292:
2276:
2270:
2264:
2261:
2256:
2246:
2237:
2233:
2227:
2224:
2219:
2210:
2202:
2198:
2191:
2185:
2180:
2170:
2166:
2159:
2155:
2150:
2144:
2138:
2133:
2119:
2111:
2107:
2103:
2100:
2097:
2091:
2085:
2080:
2076:
2072:
2066:
2060:
2057:
2052:
2047:
2041:
2035:
2032:
2020:
2014:
2011:
2008:
2005:
1992:
1991:
1990:
1976:
1947:
1941:
1938:
1935:
1932:
1920:
1918:
1902:
1882:
1862:
1842:
1833:
1820:
1817:
1812:
1808:
1800:
1797:
1785:
1759:
1755:
1747:only through
1728:
1699:
1670:
1662:
1658:
1654:
1651:
1648:
1643:
1639:
1635:
1630:
1626:
1602:
1596:
1590:
1585:
1581:
1577:
1571:
1565:
1562:
1557:
1552:
1546:
1540:
1537:
1531:
1528:
1525:
1512:
1511:
1510:
1487:
1481:
1478:
1475:
1472:
1443:
1438:
1428:
1420:
1417:
1411:
1407:
1401:
1397:
1393:
1390:
1383:
1380:
1361:
1358:
1351:
1348:
1336:
1325:
1324:
1323:
1303:
1280:
1277:
1266:
1235:
1229:
1226:
1223:
1220:
1206:
1202:
1198:
1194:
1193:supersymmetry
1179:
1176:
1166:
1163:
1160:
1157:
1148:
1146:
1130:
1127:
1124:
1121:
1115:
1112:
1106:
1103:
1079:
1076:
1064:
1057:
1052:
1048:
1027:
1024:
1021:
1018:
1015:
1012:
1009:
987:
983:
974:
958:
955:
939:
925:
922:
912:
909:
906:
903:
891:
889:
887:
871:
868:
864:
855:
848:
845:
842:
838:
829:
822:
819:
816:
811:
807:
803:
799:
790:
783:
780:
777:
774:
747:
741:
736:
726:
717:
713:
709:
703:
696:
687:
674:
666:
662:
658:
652:
646:
643:
638:
628:
621:
615:
608:
599:
590:
580:
573:
567:
561:
556:
552:
548:
542:
534:
530:
526:
521:
517:
507:
501:
495:
488:
479:
466:
460:
454:
448:
445:
442:
436:
430:
427:
415:
409:
406:
403:
400:
387:
386:
385:
371:
368:
358:
355:
352:
349:
320:
314:
311:
308:
305:
290:
288:
280:
278:
264:
261:
251:
248:
245:
242:
234:
229:
227:
226:Lorentz group
223:
219:
215:
211:
195:
192:
182:
179:
176:
173:
153:
150:
140:
137:
134:
131:
119:
117:
115:
111:
107:
103:
99:
91:
89:
87:
83:
78:
76:
72:
68:
67:superpartners
64:
59:
57:
53:
49:
45:
40:
38:
34:
30:
26:
22:
4941:Supergravity
4834:Localization
4824:Witten index
4799:Moduli space
4763:
4693:Superalgebra
4660:Supergravity
4574:
4563:
4532:
4528:
4502:
4490:. Retrieved
4470:
4466:
4456:
4424:. Retrieved
4393:
4386:
4341:
4310:
4270:
4266:
4235:
3977:
3973:
3942:
3877:, while for
3708:
3699:Fayet (1976)
3694:
3692:
3686:
3682:
3669:
3665:
3624:
3622:
3600:
3520:superpartner
3497:
3254:
3247:
3080:
2544:
2511:
2499:
2491:
2307:
2302:
2298:
2296:
1921:
1834:
1617:
1458:
1200:
1196:
1149:
940:
895:
766:
291:
284:
232:
230:
123:
114:Bruno Zumino
95:
79:
60:
43:
41:
24:
18:
5081:Researchers
5067:Stop squark
5032:Graviscalar
5027:Graviphoton
4891:WessâZumino
4754:Supercharge
4233:concisely.
4084:gauge group
4001:gauge field
3999:contains a
3216:gauge field
1205:pulled back
886:irreducible
210:gauge boson
110:Julius Wess
98:Abdus Salam
5128:Iliopoulos
5072:Superghost
5062:Sgoldstino
5047:Neutralino
4839:Mu problem
4759:R-symmetry
4723:Superspace
4718:Supergroup
4378:References
3673:, a Dirac
2335:satisfies
973:superspace
48:superspace
44:superfield
5098:Batchelor
5022:Goldstino
4911:Super QCD
4789:FI D-term
4774:BPS state
4514:1011.1491
4446:ignored (
4436:cite book
4214:ψ
4208:ϕ
4199:Φ
4176:λ
4168:μ
4066:ϕ
4046:ψ
4040:λ
4015:μ
3987:Ψ
3772:⋯
3679:auxiliary
3535:μ
3506:λ
3468:¯
3465:θ
3452:θ
3435:λ
3432:θ
3420:¯
3417:θ
3404:¯
3401:λ
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312:θ
300:Φ
235:, and in
228:changes.
86:operators
63:particles
5193:Category
5133:Montonen
5057:Sfermion
5052:R-hadron
5037:Higgsino
5012:Chargino
4901:4D N = 1
4858:Theorems
4747:Concepts
4356:See also
3549:, while
1895:, named
1293:, where
865:′
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218:graviton
75:fermions
5148:Seiberg
5123:Golfand
5103:Berezin
5088:Affleck
5017:Gaugino
4557:0416304
4537:Bibcode
4492:3 April
4475:Bibcode
4426:3 April
4399:Bibcode
3663:scalars
3597:Scalars
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92:History
52:section
42:Then a
5178:Zumino
5173:Witten
5163:Rogers
5153:Siegel
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4784:D-term
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4367:D-term
4029:, two
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767:where
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69:where
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5007:Axino
4921:NMSSM
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4509:arXiv
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4082:of a
3939:N = 2
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