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 |
|---|---|---|---|---|---|---|---|---|---|
| 455 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ | 0.5907 | 0.7264 | 0.8132 | [M:[1.0, 1.2196, 0.6706, 0.8902], q:[0.6402, 0.9696], qb:[0.3598, 0.4696], phi:[0.3902]] | [M:[[0], [2], [-3], [-1]], q:[[-1], [2]], qb:[[1], [2]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }q_{1}q_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{4}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}M_{3}q_{2}\tilde{q}_{1}$ | 0 | t^2.012 + t^2.488 + t^2.671 + t^3. + t^3.329 + 2*t^3.659 + t^3.988 + t^4.024 + t^4.317 + t^4.5 + t^4.683 + t^4.829 + t^4.976 + t^5.012 + t^5.159 + t^5.341 + t^5.488 + t^5.671 + t^5.817 + t^6.036 + 2*t^6.147 + 2*t^6.329 + t^6.476 + 2*t^6.659 + t^6.694 + t^6.806 - t^6.841 + 3*t^6.988 + t^7.024 - t^7.171 + 3*t^7.317 + t^7.353 + t^7.464 + 2*t^7.647 + t^7.683 + 3*t^7.976 + t^8.048 + 2*t^8.306 + t^8.341 + 3*t^8.635 - 2*t^8.671 + t^8.706 + t^8.817 + t^8.964 - t^4.171/y - t^6.183/y - t^6.841/y + (2*t^7.5)/y + t^7.683/y + t^8.012/y + (2*t^8.159)/y - t^8.194/y + t^8.341/y + t^8.488/y + (3*t^8.671)/y + t^8.817/y - t^8.853/y - t^4.171*y - t^6.183*y - t^6.841*y + 2*t^7.5*y + t^7.683*y + t^8.012*y + 2*t^8.159*y - t^8.194*y + t^8.341*y + t^8.488*y + 3*t^8.671*y + t^8.817*y - t^8.853*y | t^2.012/g1^3 + g1^3*t^2.488 + t^2.671/g1 + t^3. + g1*t^3.329 + 2*g1^2*t^3.659 + g1^3*t^3.988 + t^4.024/g1^6 + g1^4*t^4.317 + t^4.5 + t^4.683/g1^4 + g1*t^4.829 + g1^6*t^4.976 + t^5.012/g1^3 + g1^2*t^5.159 + t^5.341/g1^2 + g1^3*t^5.488 + t^5.671/g1 + g1^4*t^5.817 + t^6.036/g1^9 + 2*g1^5*t^6.147 + 2*g1*t^6.329 + g1^6*t^6.476 + 2*g1^2*t^6.659 + t^6.694/g1^7 + g1^7*t^6.806 - t^6.841/g1^2 + 3*g1^3*t^6.988 + t^7.024/g1^6 - t^7.171/g1 + 3*g1^4*t^7.317 + t^7.353/g1^5 + g1^9*t^7.464 + 2*g1^5*t^7.647 + t^7.683/g1^4 + 3*g1^6*t^7.976 + t^8.048/g1^12 + 2*g1^7*t^8.306 + t^8.341/g1^2 + 3*g1^8*t^8.635 - (2*t^8.671)/g1 + t^8.706/g1^10 + g1^4*t^8.817 + g1^9*t^8.964 - t^4.171/(g1*y) - t^6.183/(g1^4*y) - t^6.841/(g1^2*y) + (2*t^7.5)/y + t^7.683/(g1^4*y) + t^8.012/(g1^3*y) + (2*g1^2*t^8.159)/y - t^8.194/(g1^7*y) + t^8.341/(g1^2*y) + (g1^3*t^8.488)/y + (3*t^8.671)/(g1*y) + (g1^4*t^8.817)/y - t^8.853/(g1^5*y) - (t^4.171*y)/g1 - (t^6.183*y)/g1^4 - (t^6.841*y)/g1^2 + 2*t^7.5*y + (t^7.683*y)/g1^4 + (t^8.012*y)/g1^3 + 2*g1^2*t^8.159*y - (t^8.194*y)/g1^7 + (t^8.341*y)/g1^2 + g1^3*t^8.488*y + (3*t^8.671*y)/g1 + g1^4*t^8.817*y - (t^8.853*y)/g1^5 |
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 |
|---|---|---|---|---|---|---|---|---|
| 1846 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ | 0.6116 | 0.7678 | 0.7965 | [M:[1.0, 1.2202, 0.6698, 0.8899, 0.6698], q:[0.6399, 0.9702], qb:[0.3601, 0.4702], phi:[0.3899]] | 2*t^2.009 + t^2.491 + t^2.67 + t^3. + t^3.33 + 2*t^3.66 + 3*t^4.019 + t^4.321 + 2*t^4.5 + 2*t^4.679 + t^4.83 + t^4.981 + 2*t^5.009 + t^5.16 + 2*t^5.34 + t^5.491 + 3*t^5.67 + t^5.821 - t^6. - t^4.17/y - t^4.17*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 |
|---|---|---|---|---|---|---|---|---|---|
| 282 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}^{2}$ | 0.5924 | 0.7275 | 0.8144 | [M:[1.0, 1.2265, 0.7021, 0.845], q:[0.6159, 0.9974], qb:[0.3841, 0.4556], phi:[0.3868]] | t^2.106 + t^2.519 + t^2.535 + t^3. + t^3.214 + 2*t^3.679 + t^4.145 + t^4.213 + t^4.359 + t^4.625 + t^4.641 + t^4.84 + t^5.038 + t^5.054 + t^5.07 + t^5.106 + t^5.519 + t^5.733 + t^5.749 + t^5.786 - 2*t^6. - t^4.16/y - t^4.16*y | detail |