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 |
|---|---|---|---|---|---|---|---|---|---|
| 57377 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ | 1.2043 | 1.3871 | 0.8682 | [X:[1.2688], M:[1.4623], q:[0.7491, 0.2115], qb:[0.5197, 0.3262], phi:[0.3656]] | [X:[[0, 2]], M:[[0, -4]], q:[[-1, 8], [-1, 4]], qb:[[1, -6], [1, 0]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ 2}\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}X_{1}$ | 2 | t^2.194 + t^2.71 + t^3.226 + 2*t^3.29 + 3*t^3.806 + t^4.323 + 2*t^4.387 + 2*t^4.613 + 2*t^4.903 + 2*t^5.194 + 2*t^5.419 + t^5.484 + 2*t^5.71 + t^5.936 + 2*t^6. + 2*t^6.226 + t^6.452 + 4*t^6.516 + 3*t^6.581 + 2*t^6.806 + 4*t^7.032 + 5*t^7.097 + 2*t^7.323 + t^7.549 + 8*t^7.613 + 2*t^7.677 + 2*t^7.839 + 2*t^7.903 + 5*t^8.129 + 4*t^8.194 + 6*t^8.419 + 2*t^8.484 + 3*t^8.645 + 2*t^8.71 + 2*t^8.774 + 4*t^8.936 - t^4.097/y - t^5.194/y - t^6.29/y - t^7.323/y - (2*t^7.387)/y - t^7.903/y - t^8.484/y + t^8.936/y - t^4.097*y - t^5.194*y - t^6.29*y - t^7.323*y - 2*t^7.387*y - t^7.903*y - t^8.484*y + t^8.936*y | t^2.194/g2^2 + g2^3*t^2.71 + g2^8*t^3.226 + (2*t^3.29)/g2^3 + 3*g2^2*t^3.806 + g2^7*t^4.323 + (2*t^4.387)/g2^4 + (g1^3*t^4.613)/g2^7 + (g2^15*t^4.613)/g1^3 + 2*g2*t^4.903 + (g1^3*t^5.194)/g2^13 + (g2^9*t^5.194)/g1^3 + 2*g2^6*t^5.419 + t^5.484/g2^5 + (g1^3*t^5.71)/g2^8 + (g2^14*t^5.71)/g1^3 + g2^11*t^5.936 + 2*t^6. + (g1^3*t^6.226)/g2^3 + (g2^19*t^6.226)/g1^3 + g2^16*t^6.452 + 4*g2^5*t^6.516 + (3*t^6.581)/g2^6 + (g1^3*t^6.806)/g2^9 + (g2^13*t^6.806)/g1^3 + 4*g2^10*t^7.032 + (5*t^7.097)/g2 + (g1^3*t^7.323)/g2^4 + (g2^18*t^7.323)/g1^3 + g2^15*t^7.549 + 8*g2^4*t^7.613 + (2*t^7.677)/g2^7 + g1^3*g2*t^7.839 + (g2^23*t^7.839)/g1^3 + (g1^3*t^7.903)/g2^10 + (g2^12*t^7.903)/g1^3 + 5*g2^9*t^8.129 + (4*t^8.194)/g2^2 + (3*g1^3*t^8.419)/g2^5 + (3*g2^17*t^8.419)/g1^3 + (g1^3*t^8.484)/g2^16 + (g2^6*t^8.484)/g1^3 + 3*g2^14*t^8.645 + 2*g2^3*t^8.71 + (2*t^8.774)/g2^8 + 2*g1^3*t^8.936 + (2*g2^22*t^8.936)/g1^3 - t^4.097/(g2*y) - t^5.194/(g2^2*y) - t^6.29/(g2^3*y) - (g2^7*t^7.323)/y - (2*t^7.387)/(g2^4*y) - (g2*t^7.903)/y - t^8.484/(g2^5*y) + (g2^11*t^8.936)/y - (t^4.097*y)/g2 - (t^5.194*y)/g2^2 - (t^6.29*y)/g2^3 - g2^7*t^7.323*y - (2*t^7.387*y)/g2^4 - g2*t^7.903*y - (t^8.484*y)/g2^5 + g2^11*t^8.936*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 |
|---|---|---|---|---|---|---|---|---|
| 58471 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ | 1.2042 | 1.386 | 0.8688 | [X:[1.2727], M:[1.4545], q:[0.7576, 0.2121], qb:[0.5152, 0.3333], phi:[0.3636]] | t^2.18 + t^2.73 + 3*t^3.27 + 3*t^3.82 + 3*t^4.36 + 2*t^4.64 + 2*t^4.91 + 2*t^5.18 + 3*t^5.45 + 2*t^5.73 + 3*t^6. - t^4.09/y - t^5.18/y - t^4.09*y - t^5.18*y | detail | {a: 6411/5324, c: 7379/5324, X1: 14/11, M1: 16/11, q1: 25/33, q2: 7/33, qb1: 17/33, qb2: 1/3, phi1: 4/11} |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 47886 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.4552 | 1.6417 | 0.8864 | [X:[1.3445], M:[0.9482], q:[0.49, 0.5268], qb:[0.4916, 0.525], phi:[0.3278]] | t^2.845 + t^2.945 + t^2.95 + t^3.045 + t^3.055 + t^3.928 + t^4.028 + t^4.033 + t^4.038 + t^4.139 + t^4.911 + t^5.012 + t^5.022 + t^5.122 + t^5.504 + t^5.508 + t^5.608 + t^5.614 + t^5.689 + t^5.789 + t^5.794 + t^5.89 + t^5.895 + t^5.9 + t^5.99 + t^5.995 - 3*t^6. - t^3.983/y - t^4.967/y - t^3.983*y - t^4.967*y | detail |