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 |
|---|---|---|---|---|---|---|---|---|---|
| 55558 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ | 0.6327 | 0.784 | 0.807 | [M:[1.1845, 0.7382, 0.8155, 1.2103, 0.8412, 0.7639], q:[0.4206, 0.3948], qb:[0.8412, 0.7639], phi:[0.3948]] | [M:[[3], [12], [-3], [-2], [-8], [7]], q:[[-4], [1]], qb:[[-8], [7]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{6}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}\phi_{1}q_{1}q_{2}$ | ${}M_{3}\phi_{1}q_{2}^{2}$ | 0 | t^2.215 + t^2.292 + t^2.446 + t^2.524 + 2*t^3.554 + 2*t^3.631 + t^3.708 + t^4.429 + t^4.506 + t^4.584 + t^4.661 + 2*t^4.738 + 2*t^4.815 + t^4.893 + t^4.97 + t^5.047 + 2*t^5.768 + 3*t^5.845 + t^5.923 + 2*t^6.077 + 2*t^6.155 + t^6.232 + t^6.644 + t^6.721 + t^6.798 + 2*t^6.876 + 2*t^6.953 + 2*t^7.03 + 3*t^7.107 + 2*t^7.185 + 3*t^7.262 + 2*t^7.339 + t^7.416 + t^7.494 + t^7.571 + 2*t^7.983 + 3*t^8.06 + 2*t^8.137 + 2*t^8.369 - t^8.524 + t^8.601 + 2*t^8.678 + t^8.755 + t^8.858 + t^8.936 - t^4.185/y - t^6.399/y - t^6.476/y - t^6.708/y + t^7.506/y + (2*t^7.661)/y + (2*t^7.738)/y + t^7.815/y + t^7.893/y + (2*t^7.97)/y - t^8.614/y - t^8.691/y + t^8.768/y + (4*t^8.845)/y + (2*t^8.923)/y - t^4.185*y - t^6.399*y - t^6.476*y - t^6.708*y + t^7.506*y + 2*t^7.661*y + 2*t^7.738*y + t^7.815*y + t^7.893*y + 2*t^7.97*y - t^8.614*y - t^8.691*y + t^8.768*y + 4*t^8.845*y + 2*t^8.923*y | g1^12*t^2.215 + g1^7*t^2.292 + t^2.446/g1^3 + t^2.524/g1^8 + 2*g1^3*t^3.554 + (2*t^3.631)/g1^2 + t^3.708/g1^7 + g1^24*t^4.429 + g1^19*t^4.506 + g1^14*t^4.584 + g1^9*t^4.661 + 2*g1^4*t^4.738 + (2*t^4.815)/g1 + t^4.893/g1^6 + t^4.97/g1^11 + t^5.047/g1^16 + 2*g1^15*t^5.768 + 3*g1^10*t^5.845 + g1^5*t^5.923 + (2*t^6.077)/g1^5 + (2*t^6.155)/g1^10 + t^6.232/g1^15 + g1^36*t^6.644 + g1^31*t^6.721 + g1^26*t^6.798 + 2*g1^21*t^6.876 + 2*g1^16*t^6.953 + 2*g1^11*t^7.03 + 3*g1^6*t^7.107 + 2*g1*t^7.185 + (3*t^7.262)/g1^4 + (2*t^7.339)/g1^9 + t^7.416/g1^14 + t^7.494/g1^19 + t^7.571/g1^24 + 2*g1^27*t^7.983 + 3*g1^22*t^8.06 + 2*g1^17*t^8.137 + 2*g1^2*t^8.369 - t^8.524/g1^8 + t^8.601/g1^13 + (2*t^8.678)/g1^18 + t^8.755/g1^23 + g1^48*t^8.858 + g1^43*t^8.936 - (g1*t^4.185)/y - (g1^13*t^6.399)/y - (g1^8*t^6.476)/y - t^6.708/(g1^7*y) + (g1^19*t^7.506)/y + (2*g1^9*t^7.661)/y + (2*g1^4*t^7.738)/y + t^7.815/(g1*y) + t^7.893/(g1^6*y) + (2*t^7.97)/(g1^11*y) - (g1^25*t^8.614)/y - (g1^20*t^8.691)/y + (g1^15*t^8.768)/y + (4*g1^10*t^8.845)/y + (2*g1^5*t^8.923)/y - g1*t^4.185*y - g1^13*t^6.399*y - g1^8*t^6.476*y - (t^6.708*y)/g1^7 + g1^19*t^7.506*y + 2*g1^9*t^7.661*y + 2*g1^4*t^7.738*y + (t^7.815*y)/g1 + (t^7.893*y)/g1^6 + (2*t^7.97*y)/g1^11 - g1^25*t^8.614*y - g1^20*t^8.691*y + g1^15*t^8.768*y + 4*g1^10*t^8.845*y + 2*g1^5*t^8.923*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47126 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.639 | 0.7933 | 0.8056 | [M:[1.1493, 0.7399, 0.8507, 1.2338, 0.7924, 0.6817], q:[0.3962, 0.4545], qb:[0.8638, 0.7531], phi:[0.3831]] | t^2.045 + t^2.22 + t^2.377 + t^2.552 + t^3.448 + t^3.527 + 2*t^3.701 + t^3.876 + t^4.09 + t^4.265 + t^4.422 + t^4.44 + 2*t^4.597 + t^4.755 + t^4.772 + t^4.851 + t^4.929 + t^5.104 + t^5.493 + t^5.572 + t^5.668 + 2*t^5.746 + t^5.904 + 2*t^5.921 - 2*t^6. - t^4.149/y - t^4.149*y | detail |