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 |
|---|---|---|---|---|---|---|---|---|---|
| 6443 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{7}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{8}$ + ${ }M_{7}M_{8}$ + ${ }M_{8}M_{9}$ | 0.6622 | 0.8307 | 0.7972 | [M:[0.8959, 0.7041, 0.7521, 0.8479, 1.1521, 1.2, 0.7521, 1.2479, 0.7521], q:[0.7521, 0.3521], qb:[0.4959, 0.8], phi:[0.4]] | [M:[[2], [-2], [-1], [1], [-1], [0], [-1], [1], [-1]], q:[[-1], [-1]], qb:[[2], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{7}$, ${ }M_{9}$, ${ }M_{4}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{2}M_{9}$, ${ }M_{7}^{2}$, ${ }M_{7}M_{9}$, ${ }M_{9}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}M_{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}M_{9}$, ${ }M_{1}M_{7}$, ${ }M_{1}M_{9}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }M_{9}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{5}M_{9}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{6}M_{9}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.112 + 2*t^2.256 + t^2.544 + t^2.688 + t^3.312 + t^3.456 + t^3.6 + t^4.175 + t^4.225 + 2*t^4.369 + 4*t^4.512 + 2*t^4.656 + 2*t^4.8 + 3*t^4.944 + t^5.088 + t^5.375 + t^5.425 + 2*t^5.569 + 4*t^5.712 + 2*t^5.856 - 2*t^6. + t^6.144 + t^6.288 + t^6.337 + 2*t^6.481 + 5*t^6.625 + t^6.719 + 7*t^6.769 + t^6.863 + 4*t^6.912 + 4*t^7.056 + 4*t^7.2 + t^7.488 + t^7.537 + 3*t^7.631 + 2*t^7.681 + 6*t^7.825 + 7*t^7.969 + t^8.063 - 4*t^8.256 + t^8.35 + t^8.4 + t^8.45 - 2*t^8.544 + 2*t^8.594 - 3*t^8.688 + 5*t^8.737 + 8*t^8.881 + t^8.975 - t^4.2/y - t^6.312/y - (2*t^6.456)/y - t^6.888/y + (2*t^7.369)/y + (2*t^7.512)/y + t^7.656/y + (3*t^7.8)/y + (4*t^7.944)/y + t^8.088/y + t^8.231/y + t^8.569/y + (3*t^8.856)/y - t^4.2*y - t^6.312*y - 2*t^6.456*y - t^6.888*y + 2*t^7.369*y + 2*t^7.512*y + t^7.656*y + 3*t^7.8*y + 4*t^7.944*y + t^8.088*y + t^8.231*y + t^8.569*y + 3*t^8.856*y | t^2.112/g1^2 + (2*t^2.256)/g1 + g1*t^2.544 + g1^2*t^2.688 + t^3.312/g1^2 + t^3.456/g1 + t^3.6 + g1^4*t^4.175 + t^4.225/g1^4 + (2*t^4.369)/g1^3 + (4*t^4.512)/g1^2 + (2*t^4.656)/g1 + 2*t^4.8 + 3*g1*t^4.944 + g1^2*t^5.088 + g1^4*t^5.375 + t^5.425/g1^4 + (2*t^5.569)/g1^3 + (4*t^5.712)/g1^2 + (2*t^5.856)/g1 - 2*t^6. + g1*t^6.144 + g1^2*t^6.288 + t^6.337/g1^6 + (2*t^6.481)/g1^5 + (5*t^6.625)/g1^4 + g1^5*t^6.719 + (7*t^6.769)/g1^3 + g1^6*t^6.863 + (4*t^6.912)/g1^2 + (4*t^7.056)/g1 + 4*t^7.2 + g1^2*t^7.488 + t^7.537/g1^6 + 3*g1^3*t^7.631 + (2*t^7.681)/g1^5 + (6*t^7.825)/g1^4 + (7*t^7.969)/g1^3 + g1^6*t^8.063 - (4*t^8.256)/g1 + g1^8*t^8.35 + t^8.4 + t^8.45/g1^8 - 2*g1*t^8.544 + (2*t^8.594)/g1^7 - 3*g1^2*t^8.688 + (5*t^8.737)/g1^6 + (8*t^8.881)/g1^5 + g1^4*t^8.975 - t^4.2/y - t^6.312/(g1^2*y) - (2*t^6.456)/(g1*y) - (g1^2*t^6.888)/y + (2*t^7.369)/(g1^3*y) + (2*t^7.512)/(g1^2*y) + t^7.656/(g1*y) + (3*t^7.8)/y + (4*g1*t^7.944)/y + (g1^2*t^8.088)/y + (g1^3*t^8.231)/y + t^8.569/(g1^3*y) + (3*t^8.856)/(g1*y) - t^4.2*y - (t^6.312*y)/g1^2 - (2*t^6.456*y)/g1 - g1^2*t^6.888*y + (2*t^7.369*y)/g1^3 + (2*t^7.512*y)/g1^2 + (t^7.656*y)/g1 + 3*t^7.8*y + 4*g1*t^7.944*y + g1^2*t^8.088*y + g1^3*t^8.231*y + (t^8.569*y)/g1^3 + (3*t^8.856*y)/g1 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4825 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{7}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{8}$ + ${ }M_{7}M_{8}$ | 0.6433 | 0.7961 | 0.8081 | [M:[0.8894, 0.7106, 0.7553, 0.8447, 1.1553, 1.2, 0.7553, 1.2447], q:[0.7553, 0.3553], qb:[0.4894, 0.8], phi:[0.4]] | t^2.132 + t^2.266 + t^2.534 + t^2.668 + t^3.332 + t^3.466 + t^3.6 + t^3.734 + t^4.136 + t^4.264 + t^4.398 + 2*t^4.532 + 2*t^4.666 + t^4.8 + 2*t^4.934 + t^5.068 + t^5.336 + t^5.464 + t^5.598 + 3*t^5.732 + 2*t^5.866 - t^6. - t^4.2/y - t^4.2*y | detail |