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 |
|---|---|---|---|---|---|---|---|---|---|
| 56349 | 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_4M_5$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1q_2^2$ + $ M_7\phi_1q_1q_2$ | 0.6674 | 0.8468 | 0.7881 | [X:[], M:[1.1934, 1.0649, 0.8066, 0.8708, 1.1292, 0.7738, 0.7095], q:[0.4354, 0.3712], qb:[0.4997, 0.758], phi:[0.4839]] | [X:[], M:[[10], [-38], [-10], [14], [-14], [40], [16]], q:[[7], [-17]], qb:[[31], [3]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_7$, $ M_6$, $ M_3$, $ M_4$, $ \phi_1^2$, $ M_2$, $ M_5$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_1^2$, $ \phi_1q_2\tilde{q}_1$, $ M_7^2$, $ \phi_1q_1\tilde{q}_1$, $ M_6M_7$, $ \phi_1\tilde{q}_1^2$, $ M_3M_7$, $ M_6^2$, $ M_3M_6$, $ M_4M_7$, $ M_3^2$, $ \phi_1q_2\tilde{q}_2$, $ M_4M_6$, $ M_3M_4$, $ M_7\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_4^2$, $ M_6\phi_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2M_7$, $ M_3\phi_1^2$, $ M_2M_6$, $ M_5M_7$, $ M_4\phi_1^2$, $ M_5M_6$, $ M_1M_7$, $ M_2M_4$, $ M_3M_5$, $ \phi_1^4$, $ M_1M_6$, $ M_7\tilde{q}_1\tilde{q}_2$ | . | -1 | t^2.13 + t^2.32 + t^2.42 + t^2.61 + t^2.9 + t^3.19 + t^3.39 + t^3.58 + t^3.77 + 2*t^4.06 + 2*t^4.26 + 2*t^4.45 + t^4.55 + t^4.64 + 2*t^4.74 + t^4.84 + t^4.93 + 2*t^5.03 + 2*t^5.22 + 2*t^5.32 + 3*t^5.52 + 2*t^5.71 + t^5.81 + 2*t^5.9 - t^6. + t^6.09 + t^6.1 + t^6.19 + 5*t^6.39 + t^6.48 + 4*t^6.58 + 3*t^6.68 + 2*t^6.77 + 3*t^6.87 + t^6.96 + 3*t^6.97 + 3*t^7.06 - t^7.07 + 3*t^7.16 + t^7.25 + 4*t^7.35 + 2*t^7.45 + 2*t^7.55 + 5*t^7.64 + 6*t^7.84 + 4*t^8.03 + t^8.13 + 3*t^8.22 + t^8.23 + t^8.42 + 5*t^8.51 + t^8.52 - 2*t^8.61 + 8*t^8.71 + 2*t^8.81 + 3*t^8.9 - t^4.45/y - t^6.58/y - t^6.77/y + t^7.26/y - t^7.36/y + t^7.45/y + (2*t^7.55)/y - t^7.65/y + (2*t^7.74)/y + t^7.93/y + (2*t^8.03)/y + t^8.13/y + t^8.22/y + (3*t^8.32)/y + (3*t^8.52)/y + t^8.61/y + t^8.71/y + (2*t^8.81)/y + t^8.9/y - t^4.45*y - t^6.58*y - t^6.77*y + t^7.26*y - t^7.36*y + t^7.45*y + 2*t^7.55*y - t^7.65*y + 2*t^7.74*y + t^7.93*y + 2*t^8.03*y + t^8.13*y + t^8.22*y + 3*t^8.32*y + 3*t^8.52*y + t^8.61*y + t^8.71*y + 2*t^8.81*y + t^8.9*y | g1^16*t^2.13 + g1^40*t^2.32 + t^2.42/g1^10 + g1^14*t^2.61 + t^2.9/g1^12 + t^3.19/g1^38 + t^3.39/g1^14 + g1^10*t^3.58 + g1^34*t^3.77 + 2*g1^8*t^4.06 + 2*g1^32*t^4.26 + 2*g1^56*t^4.45 + g1^6*t^4.55 + g1^80*t^4.64 + 2*g1^30*t^4.74 + t^4.84/g1^20 + g1^54*t^4.93 + 2*g1^4*t^5.03 + 2*g1^28*t^5.22 + (2*t^5.32)/g1^22 + 3*g1^2*t^5.52 + 2*g1^26*t^5.71 + t^5.81/g1^24 + 2*g1^50*t^5.9 - t^6. + g1^74*t^6.09 + t^6.1/g1^50 + g1^24*t^6.19 + t^6.39/g1^76 + 4*g1^48*t^6.39 + t^6.48/g1^2 + t^6.58/g1^52 + 3*g1^72*t^6.58 + 3*g1^22*t^6.68 + 2*g1^96*t^6.77 + 3*g1^46*t^6.87 + g1^120*t^6.96 + (3*t^6.97)/g1^4 + 3*g1^70*t^7.06 - t^7.07/g1^54 + 3*g1^20*t^7.16 + g1^94*t^7.25 + 4*g1^44*t^7.35 + (2*t^7.45)/g1^6 + 2*g1^68*t^7.55 + 5*g1^18*t^7.64 + 6*g1^42*t^7.84 + 4*g1^66*t^8.03 + g1^16*t^8.13 + 3*g1^90*t^8.22 + t^8.23/g1^34 + g1^114*t^8.42 + 5*g1^64*t^8.51 + t^8.52/g1^60 - 2*g1^14*t^8.61 + (2*t^8.71)/g1^36 + 6*g1^88*t^8.71 + 2*g1^38*t^8.81 - t^8.9/g1^12 + 4*g1^112*t^8.9 - t^4.45/(g1^6*y) - (g1^10*t^6.58)/y - (g1^34*t^6.77)/y + (g1^32*t^7.26)/y - t^7.36/(g1^18*y) + (g1^56*t^7.45)/y + (2*g1^6*t^7.55)/y - t^7.65/(g1^44*y) + (2*g1^30*t^7.74)/y + (g1^54*t^7.93)/y + (2*g1^4*t^8.03)/y + t^8.13/(g1^46*y) + (g1^28*t^8.22)/y + (3*t^8.32)/(g1^22*y) + (3*g1^2*t^8.52)/y + t^8.61/(g1^48*y) + (g1^26*t^8.71)/y + (2*t^8.81)/(g1^24*y) + (g1^50*t^8.9)/y - (t^4.45*y)/g1^6 - g1^10*t^6.58*y - g1^34*t^6.77*y + g1^32*t^7.26*y - (t^7.36*y)/g1^18 + g1^56*t^7.45*y + 2*g1^6*t^7.55*y - (t^7.65*y)/g1^44 + 2*g1^30*t^7.74*y + g1^54*t^7.93*y + 2*g1^4*t^8.03*y + (t^8.13*y)/g1^46 + g1^28*t^8.22*y + (3*t^8.32*y)/g1^22 + 3*g1^2*t^8.52*y + (t^8.61*y)/g1^48 + g1^26*t^8.71*y + (2*t^8.81*y)/g1^24 + g1^50*t^8.9*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 |
|---|---|---|---|---|---|---|---|---|---|
| 52426 | 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_4M_5$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1q_2^2$ | 0.6471 | 0.8081 | 0.8007 | [X:[], M:[1.1947, 1.0602, 0.8053, 0.8726, 1.1274, 0.7788], q:[0.4363, 0.369], qb:[0.5035, 0.7584], phi:[0.4832]] | t^2.34 + t^2.42 + t^2.62 + t^2.9 + t^3.18 + t^3.38 + t^3.58 + t^3.79 + t^3.87 + 2*t^4.07 + t^4.27 + t^4.47 + t^4.67 + t^4.75 + t^4.83 + t^4.95 + t^5.03 + 2*t^5.24 + t^5.32 + 2*t^5.52 + t^5.72 + t^5.8 + t^5.92 - t^6. - t^4.45/y - t^4.45*y | detail |