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 |
|---|---|---|---|---|---|---|---|---|---|
| 157 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6218 | 0.7781 | 0.7992 | [M:[1.1561, 1.1561, 0.6878], q:[0.75, 0.4378], qb:[0.4061, 0.4061], phi:[0.5]] | [M:[[0, 1], [1, 0], [-1, -1]], q:[[0, 0], [-1, -1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ | -2 | t^2.063 + t^2.437 + t^3. + 4*t^3.468 + t^3.563 + 2*t^3.937 + 2*t^4.032 + 2*t^4.127 + t^4.5 + t^4.873 + t^5.063 + t^5.437 + 4*t^5.532 + t^5.627 + 2*t^5.905 - 2*t^6. + 2*t^6.19 + 2*t^6.373 + 2*t^6.468 + t^6.563 + 9*t^6.937 + 2*t^7.032 + 2*t^7.127 + t^7.31 + 4*t^7.405 + 3*t^7.5 + 6*t^7.595 + 2*t^7.69 + 3*t^7.873 + 2*t^7.968 - t^8.063 + 2*t^8.158 + 3*t^8.253 + 2*t^8.342 - 2*t^8.437 + t^8.627 + 2*t^8.81 - t^4.5/y - t^6.563/y + (2*t^7.032)/y + t^7.5/y - (2*t^7.968)/y + t^8.063/y + (2*t^8.437)/y + (4*t^8.532)/y + (4*t^8.905)/y - t^4.5*y - t^6.563*y + 2*t^7.032*y + t^7.5*y - 2*t^7.968*y + t^8.063*y + 2*t^8.437*y + 4*t^8.532*y + 4*t^8.905*y | t^2.063/(g1*g2) + g1*g2*t^2.437 + t^3. + 2*g1*t^3.468 + 2*g2*t^3.468 + t^3.563/(g1*g2) + g1^2*t^3.937 + g2^2*t^3.937 + t^4.032/g1 + t^4.032/g2 + (2*t^4.127)/(g1^2*g2^2) + t^4.5 + g1^2*g2^2*t^4.873 + t^5.063/(g1*g2) + g1*g2*t^5.437 + (2*t^5.532)/g1 + (2*t^5.532)/g2 + t^5.627/(g1^2*g2^2) + g1^2*g2*t^5.905 + g1*g2^2*t^5.905 - 2*t^6. + (2*t^6.19)/(g1^3*g2^3) + g1^3*g2*t^6.373 + g1*g2^3*t^6.373 + g1*t^6.468 + g2*t^6.468 + t^6.563/(g1*g2) + 3*g1^2*t^6.937 + 3*g1*g2*t^6.937 + 3*g2^2*t^6.937 + t^7.032/g1 + t^7.032/g2 + (2*t^7.127)/(g1^2*g2^2) + g1^3*g2^3*t^7.31 + 2*g1^3*t^7.405 + 2*g2^3*t^7.405 + t^7.5 + (g1*t^7.5)/g2 + (g2*t^7.5)/g1 + (3*t^7.595)/(g1*g2^2) + (3*t^7.595)/(g1^2*g2) + (2*t^7.69)/(g1^3*g2^3) + g1^4*t^7.873 + g1^2*g2^2*t^7.873 + g2^4*t^7.873 + (g1^2*t^7.968)/g2 + (g2^2*t^7.968)/g1 + t^8.063/g1^2 + t^8.063/g2^2 - (3*t^8.063)/(g1*g2) + t^8.158/(g1^2*g2^3) + t^8.158/(g1^3*g2^2) + (3*t^8.253)/(g1^4*g2^4) + g1^3*g2^2*t^8.342 + g1^2*g2^3*t^8.342 - 2*g1*g2*t^8.437 + t^8.627/(g1^2*g2^2) + g1^4*g2^2*t^8.81 + g1^2*g2^4*t^8.81 - t^4.5/y - t^6.563/(g1*g2*y) + t^7.032/(g1*y) + t^7.032/(g2*y) + t^7.5/y - (g1*t^7.968)/y - (g2*t^7.968)/y + t^8.063/(g1*g2*y) + (2*g1*g2*t^8.437)/y + (2*t^8.532)/(g1*y) + (2*t^8.532)/(g2*y) + (2*g1^2*g2*t^8.905)/y + (2*g1*g2^2*t^8.905)/y - t^4.5*y - (t^6.563*y)/(g1*g2) + (t^7.032*y)/g1 + (t^7.032*y)/g2 + t^7.5*y - g1*t^7.968*y - g2*t^7.968*y + (t^8.063*y)/(g1*g2) + 2*g1*g2*t^8.437*y + (2*t^8.532*y)/g1 + (2*t^8.532*y)/g2 + 2*g1^2*g2*t^8.905*y + 2*g1*g2^2*t^8.905*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 |
|---|---|---|---|---|---|---|---|---|
| 1722 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}q_{2}$ | 0.6156 | 0.7719 | 0.7976 | [M:[1.125, 1.125, 0.75], q:[0.75, 0.5], qb:[0.375, 0.375], phi:[0.5]] | 2*t^2.25 + t^3. + 4*t^3.375 + 3*t^3.75 + 2*t^4.125 + 4*t^4.5 + 2*t^5.25 + 6*t^5.625 + t^6. - t^4.5/y - t^4.5*y | detail | {a: 5043/8192, c: 6323/8192, M1: 9/8, M2: 9/8, M3: 3/4, q1: 3/4, q2: 1/2, qb1: 3/8, qb2: 3/8, phi1: 1/2} |
| 249 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ | 0.6426 | 0.819 | 0.7847 | [M:[1.1534, 1.1608, 0.6858, 0.6783], q:[0.75, 0.4358], qb:[0.4108, 0.4034], phi:[0.5]] | t^2.035 + t^2.057 + t^2.443 + t^3. + 2*t^3.46 + 2*t^3.482 + t^3.557 + t^3.92 + t^4.018 + t^4.04 + t^4.07 + t^4.092 + 2*t^4.115 + t^4.478 + t^4.5 + t^4.885 + t^5.035 + t^5.057 + t^5.443 + 2*t^5.495 + 4*t^5.518 + 2*t^5.54 + t^5.592 + t^5.615 + t^5.903 + t^5.925 + t^5.955 - 2*t^6. - t^4.5/y - t^4.5*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 |
|---|---|---|---|---|---|---|---|---|---|
| 99 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ | 0.6011 | 0.7381 | 0.8144 | [M:[1.154, 1.154], q:[0.75, 0.4419], qb:[0.404, 0.404], phi:[0.5]] | t^2.424 + t^3. + 4*t^3.462 + t^3.576 + 3*t^3.924 + 2*t^4.038 + t^4.151 + t^4.849 + t^5.424 + 2*t^5.886 - 4*t^6. - t^4.5/y - t^4.5*y | detail |