Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 46375 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ | 0.6079 | 0.7795 | 0.7799 | [M:[0.9787, 1.0638, 0.7872, 0.9787], q:[0.7447, 0.2766], qb:[0.4681, 0.4681], phi:[0.5106]] | [M:[[4], [-12], [-7], [4]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{4}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | -1 | 2*t^2.234 + t^2.362 + 2*t^2.936 + 2*t^3.192 + t^3.638 + 2*t^3.766 + 3*t^4.34 + 3*t^4.468 + 2*t^4.596 + t^4.723 + 4*t^5.17 + 2*t^5.298 + 2*t^5.426 + 2*t^5.553 + 4*t^5.872 - t^6. + 4*t^6.128 + 3*t^6.383 + 4*t^6.574 + 7*t^6.702 + t^6.83 + 4*t^6.957 + t^7.085 + 4*t^7.277 + 3*t^7.404 + 5*t^7.532 + 4*t^7.66 + 2*t^7.787 + 2*t^7.915 + t^7.979 + 7*t^8.106 - 2*t^8.234 - t^8.362 + 4*t^8.489 + 2*t^8.617 + 5*t^8.681 + 3*t^8.745 + 7*t^8.808 - 2*t^8.936 - t^4.532/y - t^6.894/y + t^7.34/y + (3*t^7.596)/y - t^7.723/y + (5*t^8.17)/y + (2*t^8.298)/y + (4*t^8.426)/y + (2*t^8.553)/y + (3*t^8.872)/y - t^4.532*y - t^6.894*y + t^7.34*y + 3*t^7.596*y - t^7.723*y + 5*t^8.17*y + 2*t^8.298*y + 4*t^8.426*y + 2*t^8.553*y + 3*t^8.872*y | 2*g1*t^2.234 + t^2.362/g1^7 + 2*g1^4*t^2.936 + (2*t^3.192)/g1^12 + g1^7*t^3.638 + (2*t^3.766)/g1 + 3*g1^10*t^4.34 + 3*g1^2*t^4.468 + (2*t^4.596)/g1^6 + t^4.723/g1^14 + 4*g1^5*t^5.17 + (2*t^5.298)/g1^3 + (2*t^5.426)/g1^11 + (2*t^5.553)/g1^19 + 4*g1^8*t^5.872 - t^6. + (4*t^6.128)/g1^8 + (3*t^6.383)/g1^24 + 4*g1^11*t^6.574 + 7*g1^3*t^6.702 + t^6.83/g1^5 + (4*t^6.957)/g1^13 + t^7.085/g1^21 + 4*g1^14*t^7.277 + 3*g1^6*t^7.404 + (5*t^7.532)/g1^2 + (4*t^7.66)/g1^10 + (2*t^7.787)/g1^18 + (2*t^7.915)/g1^26 + g1^17*t^7.979 + 7*g1^9*t^8.106 - 2*g1*t^8.234 - t^8.362/g1^7 + (4*t^8.489)/g1^15 + (2*t^8.617)/g1^23 + 5*g1^20*t^8.681 + (3*t^8.745)/g1^31 + 7*g1^12*t^8.808 - 2*g1^4*t^8.936 - t^4.532/(g1^2*y) - t^6.894/(g1^9*y) + (g1^10*t^7.34)/y + (3*t^7.596)/(g1^6*y) - t^7.723/(g1^14*y) + (5*g1^5*t^8.17)/y + (2*t^8.298)/(g1^3*y) + (4*t^8.426)/(g1^11*y) + (2*t^8.553)/(g1^19*y) + (3*g1^8*t^8.872)/y - (t^4.532*y)/g1^2 - (t^6.894*y)/g1^9 + g1^10*t^7.34*y + (3*t^7.596*y)/g1^6 - (t^7.723*y)/g1^14 + 5*g1^5*t^8.17*y + (2*t^8.298*y)/g1^3 + (4*t^8.426*y)/g1^11 + (2*t^8.553*y)/g1^19 + 3*g1^8*t^8.872*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 46105 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}^{2}$ | 0.6083 | 0.7807 | 0.7792 | [M:[0.9781, 1.0657, 0.7742, 0.9781], q:[0.7445, 0.2774], qb:[0.4812, 0.453], phi:[0.511]] | t^2.191 + t^2.276 + t^2.323 + 2*t^2.934 + 2*t^3.197 + t^3.593 + t^3.724 + t^3.809 + t^4.251 + t^4.336 + t^4.382 + t^4.42 + t^4.467 + t^4.514 + t^4.552 + t^4.599 + t^4.645 + 2*t^5.125 + 2*t^5.21 + 2*t^5.257 + t^5.388 + t^5.473 + 2*t^5.52 + t^5.784 + 3*t^5.869 + t^5.915 - 2*t^6. - t^4.533/y - t^4.533*y | detail |