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 |
|---|---|---|---|---|---|---|---|---|---|
| 46660 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ | 0.6357 | 0.8295 | 0.7663 | [M:[0.9662, 0.843, 0.8985, 0.7754], q:[0.7415, 0.2923], qb:[0.4831, 0.4154], phi:[0.5169]] | [M:[[4], [-11], [12], [-3]], q:[[1], [-5]], qb:[[2], [10]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{4}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}M_{4}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 0 | t^2.123 + 2*t^2.326 + t^2.529 + 2*t^2.696 + t^2.899 + t^3.101 + t^3.674 + t^3.877 + t^4.043 + 2*t^4.246 + 3*t^4.449 + 4*t^4.652 + 2*t^4.819 + 2*t^4.855 + 5*t^5.022 + t^5.058 + 5*t^5.225 + 3*t^5.391 + 2*t^5.428 + 2*t^5.594 + 2*t^5.797 + t^6.167 + t^6.203 + 4*t^6.369 + t^6.406 + 5*t^6.572 + 2*t^6.739 + 5*t^6.775 + 4*t^6.942 + 5*t^6.978 + 7*t^7.145 + 3*t^7.181 + 8*t^7.348 + 2*t^7.384 + 3*t^7.514 + 6*t^7.551 + t^7.587 + 8*t^7.717 + 4*t^7.754 + 7*t^7.92 + 5*t^8.087 + t^8.123 + 5*t^8.29 - 3*t^8.326 + 6*t^8.493 - 3*t^8.529 + 2*t^8.696 + 2*t^8.862 + 2*t^8.899 + t^8.935 - t^4.551/y - t^6.877/y - t^7.08/y - t^7.246/y + (2*t^7.449)/y + (2*t^7.652)/y + (2*t^7.819)/y + (3*t^7.855)/y + (6*t^8.022)/y + (6*t^8.225)/y + t^8.391/y + (3*t^8.428)/y + (2*t^8.594)/y + t^8.631/y + (3*t^8.797)/y - t^4.551*y - t^6.877*y - t^7.08*y - t^7.246*y + 2*t^7.449*y + 2*t^7.652*y + 2*t^7.819*y + 3*t^7.855*y + 6*t^8.022*y + 6*t^8.225*y + t^8.391*y + 3*t^8.428*y + 2*t^8.594*y + t^8.631*y + 3*t^8.797*y | g1^5*t^2.123 + (2*t^2.326)/g1^3 + t^2.529/g1^11 + 2*g1^12*t^2.696 + g1^4*t^2.899 + t^3.101/g1^4 + g1^3*t^3.674 + t^3.877/g1^5 + g1^18*t^4.043 + 2*g1^10*t^4.246 + 3*g1^2*t^4.449 + (4*t^4.652)/g1^6 + 2*g1^17*t^4.819 + (2*t^4.855)/g1^14 + 5*g1^9*t^5.022 + t^5.058/g1^22 + 5*g1*t^5.225 + 3*g1^24*t^5.391 + (2*t^5.428)/g1^7 + 2*g1^16*t^5.594 + 2*g1^8*t^5.797 + g1^23*t^6.167 + t^6.203/g1^8 + 4*g1^15*t^6.369 + t^6.406/g1^16 + 5*g1^7*t^6.572 + 2*g1^30*t^6.739 + (5*t^6.775)/g1 + 4*g1^22*t^6.942 + (5*t^6.978)/g1^9 + 7*g1^14*t^7.145 + (3*t^7.181)/g1^17 + 8*g1^6*t^7.348 + (2*t^7.384)/g1^25 + 3*g1^29*t^7.514 + (6*t^7.551)/g1^2 + t^7.587/g1^33 + 8*g1^21*t^7.717 + (4*t^7.754)/g1^10 + 7*g1^13*t^7.92 + 5*g1^36*t^8.087 + g1^5*t^8.123 + 5*g1^28*t^8.29 - (3*t^8.326)/g1^3 + 6*g1^20*t^8.493 - (3*t^8.529)/g1^11 + 2*g1^12*t^8.696 + 2*g1^35*t^8.862 + 2*g1^4*t^8.899 + t^8.935/g1^27 - t^4.551/(g1^2*y) - t^6.877/(g1^5*y) - t^7.08/(g1^13*y) - (g1^10*t^7.246)/y + (2*g1^2*t^7.449)/y + (2*t^7.652)/(g1^6*y) + (2*g1^17*t^7.819)/y + (3*t^7.855)/(g1^14*y) + (6*g1^9*t^8.022)/y + (6*g1*t^8.225)/y + (g1^24*t^8.391)/y + (3*t^8.428)/(g1^7*y) + (2*g1^16*t^8.594)/y + t^8.631/(g1^15*y) + (3*g1^8*t^8.797)/y - (t^4.551*y)/g1^2 - (t^6.877*y)/g1^5 - (t^7.08*y)/g1^13 - g1^10*t^7.246*y + 2*g1^2*t^7.449*y + (2*t^7.652*y)/g1^6 + 2*g1^17*t^7.819*y + (3*t^7.855*y)/g1^14 + 6*g1^9*t^8.022*y + 6*g1*t^8.225*y + g1^24*t^8.391*y + (3*t^8.428*y)/g1^7 + 2*g1^16*t^8.594*y + (t^8.631*y)/g1^15 + 3*g1^8*t^8.797*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 |
|---|---|---|---|---|---|---|---|---|
| 47274 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{5}$ | 0.6327 | 0.8239 | 0.768 | [M:[0.9706, 0.8307, 0.9119, 0.772, 1.0294], q:[0.7427, 0.2867], qb:[0.4853, 0.4266], phi:[0.5147]] | t^2.14 + 2*t^2.316 + t^2.492 + 2*t^2.736 + 2*t^3.088 + t^3.684 + t^3.86 + t^4.104 + 2*t^4.28 + 3*t^4.456 + 4*t^4.632 + 2*t^4.808 + 2*t^4.876 + t^4.984 + 4*t^5.052 + 4*t^5.228 + 3*t^5.404 + 3*t^5.471 + t^5.58 + 3*t^5.824 - t^6. - t^4.544/y - t^4.544*y | detail | |
| 47166 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.6536 | 0.8612 | 0.7589 | [M:[0.968, 0.838, 0.904, 0.774, 0.774], q:[0.742, 0.29], qb:[0.484, 0.42], phi:[0.516]] | t^2.13 + 3*t^2.322 + t^2.514 + 2*t^2.712 + t^2.904 + t^3.096 + t^3.87 + t^4.068 + 2*t^4.26 + 4*t^4.452 + 7*t^4.644 + 3*t^4.836 + 2*t^4.842 + t^5.028 + 7*t^5.034 + 6*t^5.226 + 3*t^5.418 + 3*t^5.424 + 2*t^5.616 + t^5.808 - 2*t^6. - t^4.548/y - t^4.548*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46190 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ | 0.6178 | 0.7981 | 0.7742 | [M:[0.9643, 0.8481, 0.893], q:[0.7411, 0.2946], qb:[0.4822, 0.4108], phi:[0.5178]] | t^2.116 + t^2.33 + t^2.544 + 2*t^2.679 + t^2.893 + t^3.107 + 2*t^3.67 + t^3.884 + t^4.018 + 2*t^4.232 + 2*t^4.446 + 2*t^4.661 + 2*t^4.795 + t^4.875 + 3*t^5.009 + t^5.089 + 4*t^5.223 + 3*t^5.358 + t^5.437 + 2*t^5.572 + 3*t^5.786 - t^4.554/y - t^4.554*y | detail |