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 |
|---|---|---|---|---|---|---|---|---|---|
| 46307 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | 0.6178 | 0.7527 | 0.8207 | [M:[0.7725, 1.1587, 0.8413], q:[0.8413, 0.3862], qb:[0.455, 0.7725], phi:[0.3862]] | [M:[[2], [3], [-3]], q:[[-3], [1]], qb:[[-4], [2]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | ${}M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 1 | 2*t^2.317 + t^2.524 + 2*t^3.476 + 2*t^3.683 + 2*t^3.889 + 3*t^4.635 + 3*t^4.841 + t^5.048 + 2*t^5.794 + t^6. + 4*t^6.206 + 2*t^6.413 + 5*t^6.952 + 3*t^7.159 + 3*t^7.365 + 3*t^7.571 + 3*t^7.778 + 2*t^8.111 - t^8.317 + t^8.524 + 4*t^8.73 + 2*t^8.936 - t^4.159/y - (2*t^6.476)/y + t^7.635/y + (4*t^7.841)/y + t^8.794/y - t^4.159*y - 2*t^6.476*y + t^7.635*y + 4*t^7.841*y + t^8.794*y | 2*g1^2*t^2.317 + t^2.524/g1^3 + 2*g1^3*t^3.476 + (2*t^3.683)/g1^2 + (2*t^3.889)/g1^7 + 3*g1^4*t^4.635 + (3*t^4.841)/g1 + t^5.048/g1^6 + 2*g1^5*t^5.794 + t^6. + (4*t^6.206)/g1^5 + (2*t^6.413)/g1^10 + 5*g1^6*t^6.952 + 3*g1*t^7.159 + (3*t^7.365)/g1^4 + (3*t^7.571)/g1^9 + (3*t^7.778)/g1^14 + 2*g1^7*t^8.111 - g1^2*t^8.317 + t^8.524/g1^3 + (4*t^8.73)/g1^8 + (2*t^8.936)/g1^13 - (g1*t^4.159)/y - (2*g1^3*t^6.476)/y + (g1^4*t^7.635)/y + (4*t^7.841)/(g1*y) + (g1^5*t^8.794)/y - g1*t^4.159*y - 2*g1^3*t^6.476*y + g1^4*t^7.635*y + (4*t^7.841*y)/g1 + g1^5*t^8.794*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 |
|---|---|---|---|---|---|---|---|---|
| 46637 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ | 0.632 | 0.7786 | 0.8118 | [M:[0.7817, 1.1726, 0.8274, 0.8274], q:[0.8274, 0.3909], qb:[0.4366, 0.7817], phi:[0.3909]] | 2*t^2.345 + 2*t^2.482 + t^3.518 + 2*t^3.655 + 2*t^3.792 + 3*t^4.69 + 5*t^4.827 + 3*t^4.965 + t^6. - t^4.173/y - t^4.173*y | detail | |
| 46393 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ | 0.6384 | 0.7923 | 0.8057 | [M:[0.7685, 1.1527, 0.8473, 0.6897], q:[0.8473, 0.3842], qb:[0.463, 0.7685], phi:[0.3842]] | t^2.069 + 2*t^2.305 + t^2.542 + 2*t^3.458 + 2*t^3.695 + t^3.931 + t^4.138 + 2*t^4.375 + 4*t^4.611 + 3*t^4.847 + t^5.084 + 2*t^5.527 + 4*t^5.764 + 2*t^6. - t^4.153/y - t^4.153*y | detail | |
| 46795 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ | 0.5999 | 0.7213 | 0.8316 | [M:[0.7772, 1.1658, 0.8342, 1.2228], q:[0.8342, 0.3886], qb:[0.4457, 0.7772], phi:[0.3886]] | t^2.332 + t^2.503 + 2*t^3.497 + 3*t^3.668 + 2*t^3.84 + t^4.663 + 2*t^4.834 + t^5.005 - t^4.166/y - t^4.166*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46050 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ | 0.7051 | 0.8546 | 0.8251 | [M:[0.9277, 1.0, 1.0], q:[0.6084, 0.4639], qb:[0.5361, 0.5361], phi:[0.4639]] | 2*t^2.783 + 2*t^3. + t^3.217 + 2*t^3.434 + t^4.175 + 2*t^4.392 + 4*t^4.608 + 2*t^4.825 + t^5.042 + 2*t^5.566 - t^6. - t^4.392/y - t^4.392*y | detail |