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 |
|---|---|---|---|---|---|---|---|---|---|
| 74 | SU2adj1nf2 | $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1^2$ | 0.6079 | 0.7214 | 0.8426 | [X:[], M:[0.6995, 1.2812], q:[0.8348, 0.8058], qb:[0.4657, 0.456], phi:[0.3594]] | [X:[], M:[[1, -4, -1], [0, 2, 2]], q:[[-1, 1, 1], [1, 0, 0]], qb:[[0, 3, 0], [0, 0, 3]], phi:[[0, -1, -1]]] | 3 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ \tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ M_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ q_1\tilde{q}_2$, $ M_1^2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ q_1q_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_1q_2\tilde{q}_2$, $ M_1q_2\tilde{q}_1$, $ M_1\phi_1\tilde{q}_2^2$, $ M_1M_2$, $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ | . | -3 | t^2.1 + t^2.77 + t^3.79 + 2*t^3.81 + 2*t^3.84 + 2*t^3.87 + t^4.2 + t^4.86 + t^4.92 + t^5.53 + t^5.88 + 2*t^5.91 + t^5.94 - 3*t^6. - 2*t^6.03 - t^6.06 + t^6.3 + t^6.55 + 2*t^6.58 + 2*t^6.61 + 2*t^6.64 + t^6.96 - 2*t^7.05 - 2*t^7.08 - 2*t^7.11 - t^7.14 + t^7.57 + 2*t^7.6 + 5*t^7.63 + 4*t^7.66 + 5*t^7.69 + 2*t^7.72 + 2*t^7.74 + t^7.98 + 2*t^8.01 + t^8.04 - 3*t^8.1 - 2*t^8.13 + t^8.3 + t^8.39 + t^8.65 + 2*t^8.68 + t^8.71 - 3*t^8.77 - 2*t^8.79 - 2*t^8.82 - t^4.08/y - t^6.18/y + t^7.86/y + t^7.98/y - t^8.28/y + t^8.88/y + (2*t^8.91)/y + (2*t^8.94)/y + (2*t^8.97)/y - t^4.08*y - t^6.18*y + t^7.86*y + t^7.98*y - t^8.28*y + t^8.88*y + 2*t^8.91*y + 2*t^8.94*y + 2*t^8.97*y | (g1*t^2.1)/(g2^4*g3) + g2^3*g3^3*t^2.77 + g1*g3^3*t^3.79 + g1*g2^3*t^3.81 + (g3^5*t^3.81)/g2 + 2*g2^2*g3^2*t^3.84 + (g2^5*t^3.87)/g3 + (g2*g3^4*t^3.87)/g1 + (g1^2*t^4.2)/(g2^8*g3^2) + (g1*g3^2*t^4.86)/g2 + g2*g3*t^4.92 + g2^6*g3^6*t^5.53 + (g1^2*g3^2*t^5.88)/g2^4 + (g1^2*t^5.91)/(g2*g3) + (g1*g3^4*t^5.91)/g2^5 + (g1*g3*t^5.94)/g2^2 - 3*t^6. - (g2^3*t^6.03)/g3^3 - (g3^2*t^6.03)/(g1*g2) - (g2^2*t^6.06)/(g1*g3) + (g1^3*t^6.3)/(g2^12*g3^3) + g1*g2^3*g3^6*t^6.55 + g1*g2^6*g3^3*t^6.58 + g2^2*g3^8*t^6.58 + 2*g2^5*g3^5*t^6.61 + g2^8*g3^2*t^6.64 + (g2^4*g3^7*t^6.64)/g1 + (g1^2*g3*t^6.96)/g2^5 - (g1*t^7.05)/g3^3 - (g3^2*t^7.05)/g2^4 - (2*t^7.08)/(g2*g3) - (g2^2*t^7.11)/g3^4 - (g3*t^7.11)/(g1*g2^2) - (g2*t^7.14)/(g1*g3^2) + g1^2*g3^6*t^7.57 + g1^2*g2^3*g3^3*t^7.6 + (g1*g3^8*t^7.6)/g2 + g1^2*g2^6*t^7.63 + 3*g1*g2^2*g3^5*t^7.63 + (g3^10*t^7.63)/g2^2 + 2*g1*g2^5*g3^2*t^7.66 + 2*g2*g3^7*t^7.66 + (g1*g2^8*t^7.69)/g3 + 3*g2^4*g3^4*t^7.69 + (g3^9*t^7.69)/g1 + g2^7*g3*t^7.72 + (g2^3*g3^6*t^7.72)/g1 + (g2^10*t^7.74)/g3^2 + (g2^2*g3^8*t^7.74)/g1^2 + (g1^3*g3*t^7.98)/g2^8 + (g1^3*t^8.01)/(g2^5*g3^2) + (g1^2*g3^3*t^8.01)/g2^9 + (g1^2*t^8.04)/g2^6 - (3*g1*t^8.1)/(g2^4*g3) - (g1*t^8.13)/(g2*g3^4) - (g3*t^8.13)/g2^5 + g2^9*g3^9*t^8.3 + (g1^4*t^8.39)/(g2^16*g3^4) + (g1^2*g3^5*t^8.65)/g2 + g1^2*g2^2*g3^2*t^8.68 + (g1*g3^7*t^8.68)/g2^2 + g1*g2*g3^4*t^8.71 - 3*g2^3*g3^3*t^8.77 - g2^6*t^8.79 - (g2^2*g3^5*t^8.79)/g1 - (2*g2^5*g3^2*t^8.82)/g1 - t^4.08/(g2*g3*y) - (g1*t^6.18)/(g2^5*g3^2*y) + (g1*g3^2*t^7.86)/(g2*y) + (g2^3*t^7.98)/(g1*y) - (g1^2*t^8.28)/(g2^9*g3^3*y) + (g1^2*g3^2*t^8.88)/(g2^4*y) + (g1^2*t^8.91)/(g2*g3*y) + (g1*g3^4*t^8.91)/(g2^5*y) + (2*g1*g3*t^8.94)/(g2^2*y) + (g1*g2*t^8.97)/(g3^2*y) + (g3^3*t^8.97)/(g2^3*y) - (t^4.08*y)/(g2*g3) - (g1*t^6.18*y)/(g2^5*g3^2) + (g1*g3^2*t^7.86*y)/g2 + (g2^3*t^7.98*y)/g1 - (g1^2*t^8.28*y)/(g2^9*g3^3) + (g1^2*g3^2*t^8.88*y)/g2^4 + (g1^2*t^8.91*y)/(g2*g3) + (g1*g3^4*t^8.91*y)/g2^5 + (2*g1*g3*t^8.94*y)/g2^2 + (g1*g2*t^8.97*y)/g3^2 + (g3^3*t^8.97*y)/g2^3 |
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 |
|---|---|---|---|---|---|---|---|---|
| 114 | $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3\phi_1\tilde{q}_2^2$ | 0.6281 | 0.7586 | 0.8281 | [X:[], M:[0.7009, 1.2889, 0.7009], q:[0.8375, 0.807], qb:[0.4616, 0.4718], phi:[0.3555]] | 2*t^2.1 + t^2.8 + t^3.81 + 2*t^3.84 + 2*t^3.87 + t^3.93 + 3*t^4.21 + 2*t^4.9 + t^4.93 + t^5.6 + 2*t^5.91 + 3*t^5.94 + 2*t^5.97 - 3*t^6. - t^4.07/y - t^4.07*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 |
|---|---|---|---|---|---|---|---|---|---|
| 49 | SU2adj1nf2 | $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ | 0.6281 | 0.7582 | 0.8284 | [X:[], M:[0.6941], q:[0.8347, 0.81], qb:[0.4712, 0.463], phi:[0.3553]] | t^2.08 + t^2.13 + t^2.8 + t^3.82 + 2*t^3.84 + t^3.87 + 2*t^3.89 + t^4.16 + t^4.21 + t^4.26 + t^4.88 + 2*t^4.93 + t^5.61 + t^5.9 + 2*t^5.93 + t^5.95 + 2*t^5.98 - 2*t^6. - t^4.07/y - t^4.07*y | detail |