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 |
|---|---|---|---|---|---|---|---|---|---|
| 3216 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ \phi_1^4$ + $ M_2\phi_1q_2\tilde{q}_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_1$ + $ M_4\phi_1q_2^2$ | 0.6671 | 0.8676 | 0.7689 | [X:[], M:[1.0975, 0.75, 0.75, 0.6949], q:[0.75, 0.4025], qb:[0.5, 0.3475], phi:[0.5]] | [X:[], M:[[1], [0], [0], [2]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_2$, $ M_3$, $ q_2\tilde{q}_2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1^2$, $ M_1$, $ q_1\tilde{q}_2$, $ q_1q_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ \phi_1q_2\tilde{q}_1$, $ M_2M_4$, $ M_3M_4$, $ M_4q_2\tilde{q}_2$, $ M_2^2$, $ M_2M_3$, $ M_3^2$, $ \phi_1\tilde{q}_1^2$, $ M_2q_2\tilde{q}_2$, $ M_3q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_4\phi_1^2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_2\phi_1^2$, $ M_3\phi_1^2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_1M_4$, $ M_4q_1\tilde{q}_2$, $ M_1M_2$, $ M_1M_3$, $ M_4q_1q_2$, $ M_2q_1\tilde{q}_2$, $ M_3q_1\tilde{q}_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ q_1q_2\tilde{q}_2^2$, $ M_4\phi_1\tilde{q}_2^2$, $ M_2q_1q_2$, $ M_3q_1q_2$, $ q_1q_2^2\tilde{q}_2$, $ M_2\phi_1\tilde{q}_2^2$, $ M_3\phi_1\tilde{q}_2^2$, $ q_1\tilde{q}_1\tilde{q}_2^2$, $ \phi_1q_2\tilde{q}_2^3$ | . | -2 | t^2.08 + 3*t^2.25 + t^2.54 + t^3. + 2*t^3.29 + t^3.46 + t^3.58 + t^4.04 + t^4.17 + t^4.21 + 3*t^4.33 + 7*t^4.5 + t^4.63 + 3*t^4.79 + 2*t^5.08 + 3*t^5.25 + 2*t^5.38 + 7*t^5.54 + t^5.67 + 2*t^5.71 + 4*t^5.83 - 2*t^6. + 2*t^6.13 - t^6.17 + t^6.25 + 3*t^6.29 + 3*t^6.42 + t^6.46 + 11*t^6.58 + t^6.71 + 12*t^6.75 + 5*t^6.88 + 5*t^7.04 + 3*t^7.17 - 3*t^7.21 + 6*t^7.33 + 2*t^7.46 + 4*t^7.5 + 9*t^7.63 - t^7.67 + t^7.75 + 13*t^7.79 + 4*t^7.92 + 8*t^8.08 + 2*t^8.21 - 9*t^8.25 + t^8.34 + 7*t^8.38 - 3*t^8.42 + 3*t^8.5 + 2*t^8.54 + 12*t^8.67 - t^8.71 + t^8.8 + 20*t^8.83 + 5*t^8.96 - t^4.5/y - t^6.58/y - (2*t^6.75)/y + t^7.21/y + (3*t^7.33)/y + (3*t^7.5)/y + t^7.63/y + (2*t^7.79)/y + t^8.08/y + (5*t^8.25)/y + (2*t^8.38)/y + t^8.42/y + (8*t^8.54)/y + (3*t^8.71)/y + (3*t^8.83)/y - t^4.5*y - t^6.58*y - 2*t^6.75*y + t^7.21*y + 3*t^7.33*y + 3*t^7.5*y + t^7.63*y + 2*t^7.79*y + t^8.08*y + 5*t^8.25*y + 2*t^8.38*y + t^8.42*y + 8*t^8.54*y + 3*t^8.71*y + 3*t^8.83*y | g1^2*t^2.08 + 3*t^2.25 + g1*t^2.54 + t^3. + 2*g1*t^3.29 + t^3.46/g1 + g1^2*t^3.58 + g1*t^4.04 + g1^4*t^4.17 + t^4.21/g1 + 3*g1^2*t^4.33 + 7*t^4.5 + g1^3*t^4.63 + 3*g1*t^4.79 + 2*g1^2*t^5.08 + 3*t^5.25 + 2*g1^3*t^5.38 + 7*g1*t^5.54 + g1^4*t^5.67 + (2*t^5.71)/g1 + 4*g1^2*t^5.83 - 2*t^6. + 2*g1^3*t^6.13 - t^6.17/g1^2 + g1^6*t^6.25 + 3*g1*t^6.29 + 3*g1^4*t^6.42 + t^6.46/g1 + 11*g1^2*t^6.58 + g1^5*t^6.71 + 12*t^6.75 + 5*g1^3*t^6.88 + 5*g1*t^7.04 + 3*g1^4*t^7.17 - (3*t^7.21)/g1 + 6*g1^2*t^7.33 + 2*g1^5*t^7.46 + 4*t^7.5 + 9*g1^3*t^7.63 - t^7.67/g1^2 + g1^6*t^7.75 + 13*g1*t^7.79 + 4*g1^4*t^7.92 + 8*g1^2*t^8.08 + 2*g1^5*t^8.21 - 9*t^8.25 + g1^8*t^8.34 + 7*g1^3*t^8.38 - (3*t^8.42)/g1^2 + 3*g1^6*t^8.5 + 2*g1*t^8.54 + 12*g1^4*t^8.67 - t^8.71/g1 + g1^7*t^8.8 + 20*g1^2*t^8.83 + 5*g1^5*t^8.96 - t^4.5/y - (g1^2*t^6.58)/y - (2*t^6.75)/y + t^7.21/(g1*y) + (3*g1^2*t^7.33)/y + (3*t^7.5)/y + (g1^3*t^7.63)/y + (2*g1*t^7.79)/y + (g1^2*t^8.08)/y + (5*t^8.25)/y + (2*g1^3*t^8.38)/y + t^8.42/(g1^2*y) + (8*g1*t^8.54)/y + (3*t^8.71)/(g1*y) + (3*g1^2*t^8.83)/y - t^4.5*y - g1^2*t^6.58*y - 2*t^6.75*y + (t^7.21*y)/g1 + 3*g1^2*t^7.33*y + 3*t^7.5*y + g1^3*t^7.63*y + 2*g1*t^7.79*y + g1^2*t^8.08*y + 5*t^8.25*y + 2*g1^3*t^8.38*y + (t^8.42*y)/g1^2 + 8*g1*t^8.54*y + (3*t^8.71*y)/g1 + 3*g1^2*t^8.83*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2709 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ \phi_1^4$ + $ M_2\phi_1q_2\tilde{q}_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_1$ | 0.6466 | 0.8276 | 0.7814 | [X:[], M:[1.105, 0.75, 0.75], q:[0.75, 0.395], qb:[0.5, 0.355], phi:[0.5]] | 3*t^2.25 + t^2.56 + t^3. + 2*t^3.31 + t^3.44 + t^3.63 + t^3.87 + t^4.06 + t^4.19 + 7*t^4.5 + 3*t^4.81 + t^5.13 + 3*t^5.25 + 6*t^5.56 + 2*t^5.69 + 4*t^5.88 - 2*t^6. - t^4.5/y - t^4.5*y | detail |