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 |
|---|---|---|---|---|---|---|---|---|---|
| 56132 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_5q_2\tilde{q}_1$ + $ M_2M_5$ + $ M_5M_6$ + $ \phi_1\tilde{q}_2^2$ + $ M_7\phi_1q_1q_2$ | 0.6814 | 0.8529 | 0.7989 | [X:[], M:[1.1584, 1.0367, 0.8416, 0.7681, 0.9633, 1.0367, 0.7072], q:[0.384, 0.4575], qb:[0.5792, 0.7744], phi:[0.4512]] | [X:[], M:[[-14], [22], [14], [-30], [-22], [22], [-12]], q:[[-15], [29]], qb:[[-7], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_7$, $ M_4$, $ M_3$, $ \phi_1^2$, $ M_2$, $ M_6$, $ M_1$, $ \phi_1q_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ M_7^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4M_7$, $ \phi_1q_2\tilde{q}_1$, $ M_4^2$, $ M_3M_7$, $ M_3M_4$, $ M_7\phi_1^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_4\phi_1^2$, $ M_3^2$, $ \phi_1q_2\tilde{q}_2$, $ M_2M_7$, $ M_6M_7$, $ M_3\phi_1^2$, $ M_2M_4$, $ M_4M_6$, $ \phi_1^4$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1M_7$, $ M_2M_3$, $ M_3M_6$, $ M_1M_4$, $ M_7\phi_1q_1^2$, $ M_2\phi_1^2$, $ M_6\phi_1^2$, $ M_4\phi_1q_1^2$ | . | -2 | t^2.12 + t^2.3 + t^2.52 + t^2.71 + 2*t^3.11 + t^3.48 + t^3.66 + t^4.06 + t^4.1 + 2*t^4.24 + t^4.43 + t^4.46 + t^4.61 + t^4.65 + 3*t^4.83 + t^5.01 + t^5.05 + 3*t^5.23 + 2*t^5.41 + t^5.6 + t^5.63 + t^5.78 + 2*t^5.82 + t^5.96 - 2*t^6. + 2*t^6.18 + 3*t^6.22 + 3*t^6.37 + 2*t^6.55 + t^6.59 + t^6.62 + t^6.73 + 3*t^6.77 + t^6.81 + t^6.91 + 3*t^6.95 - t^6.99 + 3*t^7.13 + 2*t^7.17 + 2*t^7.21 + 2*t^7.32 + 3*t^7.35 - t^7.39 + 4*t^7.54 + 2*t^7.57 + 3*t^7.72 + t^7.76 + 2*t^7.9 + 3*t^7.94 + t^8.08 - t^8.12 + t^8.16 + t^8.2 + t^8.27 + 3*t^8.34 + 4*t^8.49 + t^8.52 + t^8.56 + 3*t^8.67 - 2*t^8.71 + t^8.75 + 2*t^8.85 + 2*t^8.89 + 4*t^8.93 - t^4.35/y - t^6.48/y - t^6.66/y - t^7.06/y + t^7.24/y + t^7.43/y - t^7.46/y + (2*t^7.65)/y + (2*t^7.83)/y + t^8.01/y + t^8.05/y + (4*t^8.23)/y + (2*t^8.41)/y + (2*t^8.63)/y + t^8.78/y + (2*t^8.82)/y - t^4.35*y - t^6.48*y - t^6.66*y - t^7.06*y + t^7.24*y + t^7.43*y - t^7.46*y + 2*t^7.65*y + 2*t^7.83*y + t^8.01*y + t^8.05*y + 4*t^8.23*y + 2*t^8.41*y + 2*t^8.63*y + t^8.78*y + 2*t^8.82*y | t^2.12/g1^12 + t^2.3/g1^30 + g1^14*t^2.52 + t^2.71/g1^4 + 2*g1^22*t^3.11 + t^3.48/g1^14 + t^3.66/g1^32 + t^4.06/g1^6 + g1^56*t^4.1 + (2*t^4.24)/g1^24 + t^4.43/g1^42 + g1^20*t^4.46 + t^4.61/g1^60 + g1^2*t^4.65 + (3*t^4.83)/g1^16 + t^5.01/g1^34 + g1^28*t^5.05 + 3*g1^10*t^5.23 + (2*t^5.41)/g1^8 + t^5.6/g1^26 + g1^36*t^5.63 + t^5.78/g1^44 + 2*g1^18*t^5.82 + t^5.96/g1^62 - 2*t^6. + (2*t^6.18)/g1^18 + 3*g1^44*t^6.22 + (3*t^6.37)/g1^36 + (2*t^6.55)/g1^54 + g1^8*t^6.59 + g1^70*t^6.62 + t^6.73/g1^72 + (3*t^6.77)/g1^10 + g1^52*t^6.81 + t^6.91/g1^90 + (3*t^6.95)/g1^28 - g1^34*t^6.99 + (3*t^7.13)/g1^46 + 2*g1^16*t^7.17 + 2*g1^78*t^7.21 + (2*t^7.32)/g1^64 + (3*t^7.35)/g1^2 - g1^60*t^7.39 + (4*t^7.54)/g1^20 + 2*g1^42*t^7.57 + (3*t^7.72)/g1^38 + g1^24*t^7.76 + (2*t^7.9)/g1^56 + 3*g1^6*t^7.94 + t^8.08/g1^74 - t^8.12/g1^12 + g1^50*t^8.16 + g1^112*t^8.2 + t^8.27/g1^92 + 3*g1^32*t^8.34 + (4*t^8.49)/g1^48 + g1^14*t^8.52 + g1^76*t^8.56 + (3*t^8.67)/g1^66 - (2*t^8.71)/g1^4 + g1^58*t^8.75 + (2*t^8.85)/g1^84 + (2*t^8.89)/g1^22 + 4*g1^40*t^8.93 - t^4.35/(g1^2*y) - t^6.48/(g1^14*y) - t^6.66/(g1^32*y) - t^7.06/(g1^6*y) + t^7.24/(g1^24*y) + t^7.43/(g1^42*y) - (g1^20*t^7.46)/y + (2*g1^2*t^7.65)/y + (2*t^7.83)/(g1^16*y) + t^8.01/(g1^34*y) + (g1^28*t^8.05)/y + (4*g1^10*t^8.23)/y + (2*t^8.41)/(g1^8*y) + (2*g1^36*t^8.63)/y + t^8.78/(g1^44*y) + (2*g1^18*t^8.82)/y - (t^4.35*y)/g1^2 - (t^6.48*y)/g1^14 - (t^6.66*y)/g1^32 - (t^7.06*y)/g1^6 + (t^7.24*y)/g1^24 + (t^7.43*y)/g1^42 - g1^20*t^7.46*y + 2*g1^2*t^7.65*y + (2*t^7.83*y)/g1^16 + (t^8.01*y)/g1^34 + g1^28*t^8.05*y + 4*g1^10*t^8.23*y + (2*t^8.41*y)/g1^8 + 2*g1^36*t^8.63*y + (t^8.78*y)/g1^44 + 2*g1^18*t^8.82*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50873 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_5q_2\tilde{q}_1$ + $ M_2M_5$ + $ M_5M_6$ + $ \phi_1\tilde{q}_2^2$ | 0.661 | 0.8142 | 0.8118 | [X:[], M:[1.1599, 1.0344, 0.8401, 0.7713, 0.9656, 1.0344], q:[0.3856, 0.4544], qb:[0.58, 0.7743], phi:[0.4514]] | t^2.31 + t^2.52 + t^2.71 + 2*t^3.1 + t^3.48 + t^3.67 + t^3.87 + t^4.06 + t^4.08 + t^4.25 + t^4.46 + t^4.63 + 2*t^4.83 + t^5.02 + t^5.04 + t^5.23 + 2*t^5.42 + t^5.62 + 2*t^5.81 + t^5.98 - 2*t^6. - t^4.35/y - t^4.35*y | detail |