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 |
|---|---|---|---|---|---|---|---|---|---|
| 391 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ \phi_1^4$ + $ M_2q_2\tilde{q}_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_3\phi_1\tilde{q}_2^2$ + $ M_3M_4$ | 0.6011 | 0.7381 | 0.8144 | [X:[], M:[1.154, 1.154, 0.6919, 1.3081], q:[0.75, 0.4419], qb:[0.404, 0.404], phi:[0.5]] | [X:[], M:[[1], [1], [-2], [2]], q:[[0], [-2]], qb:[[1], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $\tilde{q}_1\tilde{q}_2$, $ \phi_1^2$, $ M_1$, $ M_2$, $ q_1\tilde{q}_1$, $ q_1\tilde{q}_2$, $ q_1q_2$, $ M_4$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ \phi_1^2\tilde{q}_1\tilde{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$ | . | -4 | t^2.42 + t^3. + 4*t^3.46 + t^3.58 + 3*t^3.92 + 2*t^4.04 + t^4.15 + t^4.85 + t^5.42 + 2*t^5.89 - 4*t^6. - 2*t^6.11 + 3*t^6.35 + 2*t^6.46 + 9*t^6.92 + 2*t^7.04 + t^7.15 + t^7.27 + 8*t^7.39 + 3*t^7.5 + 2*t^7.61 + t^7.73 + 6*t^7.85 + 2*t^7.96 + 2*t^8.08 + 2*t^8.19 + t^8.3 + 2*t^8.31 - 4*t^8.42 - 2*t^8.54 + 3*t^8.77 - t^4.5/y + (2*t^7.04)/y - (2*t^7.96)/y + t^8.42/y + (4*t^8.89)/y - t^4.5*y + 2*t^7.04*y - 2*t^7.96*y + t^8.42*y + 4*t^8.89*y | g1^2*t^2.42 + t^3. + 4*g1*t^3.46 + t^3.58/g1^2 + 3*g1^2*t^3.92 + (2*t^4.04)/g1 + t^4.15/g1^4 + g1^4*t^4.85 + g1^2*t^5.42 + 2*g1^3*t^5.89 - 4*t^6. - (2*t^6.11)/g1^3 + 3*g1^4*t^6.35 + 2*g1*t^6.46 + 9*g1^2*t^6.92 + (2*t^7.04)/g1 + t^7.15/g1^4 + g1^6*t^7.27 + 8*g1^3*t^7.39 + 3*t^7.5 + (2*t^7.61)/g1^3 + t^7.73/g1^6 + 6*g1^4*t^7.85 + 2*g1*t^7.96 + (2*t^8.08)/g1^2 + (2*t^8.19)/g1^5 + t^8.3/g1^8 + 2*g1^5*t^8.31 - 4*g1^2*t^8.42 - (2*t^8.54)/g1 + 3*g1^6*t^8.77 - t^4.5/y + (2*t^7.04)/(g1*y) - (2*g1*t^7.96)/y + (g1^2*t^8.42)/y + (4*g1^3*t^8.89)/y - t^4.5*y + (2*t^7.04*y)/g1 - 2*g1*t^7.96*y + g1^2*t^8.42*y + 4*g1^3*t^8.89*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 247 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ \phi_1^4$ + $ M_2q_2\tilde{q}_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_3\phi_1\tilde{q}_2^2$ | 0.6218 | 0.7781 | 0.7992 | [X:[], M:[1.1561, 1.1561, 0.6878], q:[0.75, 0.4378], qb:[0.4061, 0.4061], phi:[0.5]] | t^2.06 + t^2.44 + t^3. + 4*t^3.47 + t^3.56 + 2*t^3.94 + 2*t^4.03 + 2*t^4.13 + t^4.5 + t^4.87 + t^5.06 + t^5.44 + 4*t^5.53 + t^5.63 + 2*t^5.91 - 2*t^6. - t^4.5/y - t^4.5*y | detail |