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 |
|---|---|---|---|---|---|---|---|---|---|
| 1141 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ | 0.6732 | 0.8376 | 0.8036 | [M:[0.9644, 1.0879, 1.1401, 0.8599, 0.8599, 0.7364], q:[0.772, 0.5439], qb:[0.4917, 0.3682], phi:[0.4561]] | [M:[[13], [-4], [5], [-5], [-5], [12]], q:[[-1], [-2]], qb:[[-11], [6]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$ | ${}$ | -2 | t^2.209 + 2*t^2.58 + t^2.736 + t^2.893 + t^3.264 + t^3.577 + 2*t^3.948 + t^4.105 + t^4.318 + t^4.418 + t^4.475 + t^4.632 + 2*t^4.789 + t^4.945 + t^5.102 + 3*t^5.159 + 2*t^5.316 + 3*t^5.473 + 2*t^5.786 + t^5.843 - 2*t^6. + 3*t^6.157 + 2*t^6.314 - t^6.371 + t^6.47 + 3*t^6.527 + t^6.627 + 2*t^6.684 + 2*t^6.841 + 2*t^6.898 + 2*t^6.998 + 2*t^7.055 + 2*t^7.154 + 2*t^7.211 + t^7.311 + 2*t^7.368 + 3*t^7.525 + 4*t^7.682 + 2*t^7.739 + 3*t^7.895 + 2*t^7.995 + 4*t^8.052 - t^8.209 + t^8.266 + 4*t^8.366 + t^8.423 + 2*t^8.523 - 5*t^8.58 + t^8.636 + 2*t^8.679 + 2*t^8.736 + t^8.793 + t^8.836 - t^8.95 - t^4.368/y - t^6.577/y - t^6.948/y - t^7.261/y + t^7.475/y + (3*t^7.789)/y + t^7.945/y + t^8.102/y + (2*t^8.159)/y + (2*t^8.316)/y + (3*t^8.473)/y + t^8.629/y + (2*t^8.843)/y - t^4.368*y - t^6.577*y - t^6.948*y - t^7.261*y + t^7.475*y + 3*t^7.789*y + t^7.945*y + t^8.102*y + 2*t^8.159*y + 2*t^8.316*y + 3*t^8.473*y + t^8.629*y + 2*t^8.843*y | g1^12*t^2.209 + (2*t^2.58)/g1^5 + g1^4*t^2.736 + g1^13*t^2.893 + t^3.264/g1^4 + g1^14*t^3.577 + (2*t^3.948)/g1^3 + g1^6*t^4.105 + t^4.318/g1^20 + g1^24*t^4.418 + t^4.475/g1^11 + t^4.632/g1^2 + 2*g1^7*t^4.789 + g1^16*t^4.945 + g1^25*t^5.102 + (3*t^5.159)/g1^10 + (2*t^5.316)/g1 + 3*g1^8*t^5.473 + 2*g1^26*t^5.786 + t^5.843/g1^9 - 2*t^6. + 3*g1^9*t^6.157 + 2*g1^18*t^6.314 - t^6.371/g1^17 + g1^27*t^6.47 + (3*t^6.527)/g1^8 + g1^36*t^6.627 + 2*g1*t^6.684 + 2*g1^10*t^6.841 + (2*t^6.898)/g1^25 + 2*g1^19*t^6.998 + (2*t^7.055)/g1^16 + 2*g1^28*t^7.154 + (2*t^7.211)/g1^7 + g1^37*t^7.311 + 2*g1^2*t^7.368 + 3*g1^11*t^7.525 + 4*g1^20*t^7.682 + (2*t^7.739)/g1^15 + (3*t^7.895)/g1^6 + 2*g1^38*t^7.995 + 4*g1^3*t^8.052 - g1^12*t^8.209 + t^8.266/g1^23 + 4*g1^21*t^8.366 + t^8.423/g1^14 + 2*g1^30*t^8.523 - (5*t^8.58)/g1^5 + t^8.636/g1^40 + 2*g1^39*t^8.679 + 2*g1^4*t^8.736 + t^8.793/g1^31 + g1^48*t^8.836 - t^8.95/g1^22 - (g1^2*t^4.368)/y - (g1^14*t^6.577)/y - t^6.948/(g1^3*y) - (g1^15*t^7.261)/y + t^7.475/(g1^11*y) + (3*g1^7*t^7.789)/y + (g1^16*t^7.945)/y + (g1^25*t^8.102)/y + (2*t^8.159)/(g1^10*y) + (2*t^8.316)/(g1*y) + (3*g1^8*t^8.473)/y + (g1^17*t^8.629)/y + (2*t^8.843)/(g1^9*y) - g1^2*t^4.368*y - g1^14*t^6.577*y - (t^6.948*y)/g1^3 - g1^15*t^7.261*y + (t^7.475*y)/g1^11 + 3*g1^7*t^7.789*y + g1^16*t^7.945*y + g1^25*t^8.102*y + (2*t^8.159*y)/g1^10 + (2*t^8.316*y)/g1 + 3*g1^8*t^8.473*y + g1^17*t^8.629*y + (2*t^8.843*y)/g1^9 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 702 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{5}$ | 0.6539 | 0.8024 | 0.8149 | [M:[0.9817, 1.0826, 1.1468, 0.8532, 0.8532], q:[0.7706, 0.5413], qb:[0.477, 0.3762], phi:[0.4587]] | 2*t^2.56 + t^2.752 + t^2.945 + t^3.248 + t^3.633 + t^3.743 + 2*t^3.936 + t^4.128 + t^4.238 + t^4.431 + t^4.624 + 3*t^5.119 + 2*t^5.312 + 2*t^5.505 + t^5.807 + t^5.89 - 2*t^6. - t^4.376/y - t^4.376*y | detail |