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 |
|---|---|---|---|---|---|---|---|---|---|
| 55383 | 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_2^2$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ + $ M_4X_1$ + $ M_5\phi_1q_2^2$ + $ M_1M_6$ | 0.6122 | 0.774 | 0.7909 | [X:[1.3578], M:[1.2316, 1.0, 0.7684, 0.6422, 0.6949, 0.7684], q:[0.3211, 0.4473], qb:[0.6789, 0.9105], phi:[0.4105]] | [X:[[4]], M:[[-3], [0], [3], [-4], [-9], [3]], q:[[-2], [5]], qb:[[2], [-1]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ M_3$, $ M_6$, $ \phi_1^2$, $ M_2$, $ \phi_1q_1^2$, $ q_2\tilde{q}_1$, $ \phi_1q_1q_2$, $ X_1$, $ M_5^2$, $ M_3M_5$, $ M_5M_6$, $ M_5\phi_1^2$, $ M_3^2$, $ M_3M_6$, $ M_6^2$, $ \phi_1q_2\tilde{q}_1$, $ M_3\phi_1^2$, $ M_6\phi_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1^4$, $ \phi_1q_1\tilde{q}_2$, $ M_2M_5$, $ M_5\phi_1q_1^2$, $ M_2M_3$, $ M_2M_6$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_2\phi_1^2$, $ M_6\phi_1q_1^2$, $ M_5q_2\tilde{q}_1$, $ \phi_1^3q_1^2$, $ M_5\phi_1q_1q_2$, $ M_3q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ M_6\phi_1q_1q_2$, $ \phi_1^2q_2\tilde{q}_1$ | $\phi_1^3q_1q_2$ | -1 | t^2.08 + 2*t^2.31 + t^2.46 + t^3. + t^3.16 + t^3.38 + t^3.54 + t^4.07 + t^4.17 + 2*t^4.39 + t^4.55 + 3*t^4.61 + 3*t^4.77 + t^4.93 + t^5.08 + t^5.24 + 2*t^5.31 + 3*t^5.46 + t^5.62 + 2*t^5.68 + 2*t^5.84 - t^6. + t^6.16 + t^6.25 + t^6.32 + 2*t^6.38 + 2*t^6.47 + t^6.54 + t^6.63 + 2*t^6.69 + t^6.76 + 2*t^6.85 + 4*t^6.92 + t^7.01 + 3*t^7.07 + t^7.17 + t^7.23 + t^7.33 + 2*t^7.39 + 3*t^7.55 + 2*t^7.61 + t^7.71 + 4*t^7.77 + 2*t^7.93 + 3*t^7.99 - t^8.08 + 4*t^8.15 + t^8.24 - 3*t^8.31 + t^8.34 + t^8.4 + 2*t^8.56 + t^8.62 + 2*t^8.68 + t^8.72 + 2*t^8.78 + t^8.84 + 2*t^8.94 - t^4.23/y - t^6.32/y - t^6.54/y - t^6.69/y + (2*t^7.39)/y + t^7.55/y + t^7.61/y + (3*t^7.77)/y + t^7.93/y + t^8.08/y + t^8.15/y + t^8.24/y + (2*t^8.31)/y - t^8.4/y + (4*t^8.46)/y + t^8.62/y + (2*t^8.68)/y - t^8.78/y + (2*t^8.84)/y - t^4.23*y - t^6.32*y - t^6.54*y - t^6.69*y + 2*t^7.39*y + t^7.55*y + t^7.61*y + 3*t^7.77*y + t^7.93*y + t^8.08*y + t^8.15*y + t^8.24*y + 2*t^8.31*y - t^8.4*y + 4*t^8.46*y + t^8.62*y + 2*t^8.68*y - t^8.78*y + 2*t^8.84*y | t^2.08/g1^9 + 2*g1^3*t^2.31 + t^2.46/g1^2 + t^3. + t^3.16/g1^5 + g1^7*t^3.38 + g1^2*t^3.54 + g1^4*t^4.07 + t^4.17/g1^18 + (2*t^4.39)/g1^6 + t^4.55/g1^11 + 3*g1^6*t^4.61 + 3*g1*t^4.77 + t^4.93/g1^4 + t^5.08/g1^9 + t^5.24/g1^14 + 2*g1^3*t^5.31 + (3*t^5.46)/g1^2 + t^5.62/g1^7 + 2*g1^10*t^5.68 + 2*g1^5*t^5.84 - t^6. + t^6.16/g1^5 + t^6.25/g1^27 + t^6.32/g1^10 + 2*g1^7*t^6.38 + (2*t^6.47)/g1^15 + g1^2*t^6.54 + t^6.63/g1^20 + (2*t^6.69)/g1^3 + g1^14*t^6.76 + (2*t^6.85)/g1^8 + 4*g1^9*t^6.92 + t^7.01/g1^13 + 3*g1^4*t^7.07 + t^7.17/g1^18 + t^7.23/g1 + t^7.33/g1^23 + (2*t^7.39)/g1^6 + (3*t^7.55)/g1^11 + 2*g1^6*t^7.61 + t^7.71/g1^16 + 4*g1*t^7.77 + (2*t^7.93)/g1^4 + 3*g1^13*t^7.99 - t^8.08/g1^9 + 4*g1^8*t^8.15 + t^8.24/g1^14 - 3*g1^3*t^8.31 + t^8.34/g1^36 + t^8.4/g1^19 + (2*t^8.56)/g1^24 + t^8.62/g1^7 + 2*g1^10*t^8.68 + t^8.72/g1^29 + (2*t^8.78)/g1^12 + g1^5*t^8.84 + (2*t^8.94)/g1^17 - t^4.23/(g1*y) - t^6.32/(g1^10*y) - (g1^2*t^6.54)/y - t^6.69/(g1^3*y) + (2*t^7.39)/(g1^6*y) + t^7.55/(g1^11*y) + (g1^6*t^7.61)/y + (3*g1*t^7.77)/y + t^7.93/(g1^4*y) + t^8.08/(g1^9*y) + (g1^8*t^8.15)/y + t^8.24/(g1^14*y) + (2*g1^3*t^8.31)/y - t^8.4/(g1^19*y) + (4*t^8.46)/(g1^2*y) + t^8.62/(g1^7*y) + (2*g1^10*t^8.68)/y - t^8.78/(g1^12*y) + (2*g1^5*t^8.84)/y - (t^4.23*y)/g1 - (t^6.32*y)/g1^10 - g1^2*t^6.54*y - (t^6.69*y)/g1^3 + (2*t^7.39*y)/g1^6 + (t^7.55*y)/g1^11 + g1^6*t^7.61*y + 3*g1*t^7.77*y + (t^7.93*y)/g1^4 + (t^8.08*y)/g1^9 + g1^8*t^8.15*y + (t^8.24*y)/g1^14 + 2*g1^3*t^8.31*y - (t^8.4*y)/g1^19 + (4*t^8.46*y)/g1^2 + (t^8.62*y)/g1^7 + 2*g1^10*t^8.68*y - (t^8.78*y)/g1^12 + 2*g1^5*t^8.84*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46972 | 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_2^2$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ + $ M_4X_1$ + $ M_5\phi_1q_2^2$ | 0.5941 | 0.7418 | 0.8009 | [X:[1.3633], M:[1.2275, 1.0, 0.7725, 0.6367, 0.6825], q:[0.3183, 0.4541], qb:[0.6817, 0.9092], phi:[0.4092]] | t^2.05 + t^2.32 + t^2.46 + t^3. + t^3.14 + t^3.41 + t^3.54 + t^3.68 + t^4.09 + t^4.1 + t^4.37 + t^4.5 + t^4.63 + 2*t^4.77 + t^4.91 + t^5.05 + t^5.19 + t^5.32 + 2*t^5.46 + t^5.59 + t^5.72 + t^5.73 + t^5.86 - t^4.23/y - t^4.23*y | detail |