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 |
|---|---|---|---|---|---|---|---|---|---|
| 3187 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ M_1M_3$ + $ M_3M_6$ + $ \phi_1q_1\tilde{q}_2$ + $ M_7\phi_1q_2^2$ | 0.5963 | 0.759 | 0.7856 | [X:[], M:[0.9827, 0.7415, 1.0173, 0.7069, 1.2931, 0.9827, 0.8275], q:[0.6466, 0.3707], qb:[0.3361, 0.9224], phi:[0.431]] | [X:[], M:[[14], [-22], [-14], [6], [-6], [14], [24]], q:[[-3], [-11]], qb:[[17], [5]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_2$, $ M_7$, $ \phi_1^2$, $ M_1$, $ M_6$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_1$, $ M_5$, $ M_4^2$, $ \phi_1q_1\tilde{q}_1$, $ M_2M_4$, $ \phi_1q_1q_2$, $ M_2^2$, $ M_4M_7$, $ M_2M_7$, $ M_4\phi_1^2$, $ q_1\tilde{q}_2$, $ M_2\phi_1^2$, $ M_7^2$, $ M_1M_4$, $ M_4M_6$, $ M_7\phi_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1M_2$, $ M_2M_6$, $ \phi_1^4$, $ \phi_1q_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_1M_7$, $ M_6M_7$, $ M_4\phi_1\tilde{q}_1^2$, $ M_1\phi_1^2$, $ M_6\phi_1^2$, $ M_4\phi_1q_2\tilde{q}_1$, $ M_7\phi_1\tilde{q}_1^2$, $ M_1^2$, $ M_1M_6$, $ M_6^2$, $ M_7\phi_1q_2\tilde{q}_1$, $ \phi_1^3\tilde{q}_1^2$ | $\phi_1^3q_2\tilde{q}_1$ | -1 | t^2.12 + t^2.22 + t^2.48 + t^2.59 + 2*t^2.95 + t^3.31 + t^3.41 + t^3.88 + t^4.24 + t^4.35 + t^4.45 + t^4.6 + 3*t^4.71 + t^4.81 + t^4.96 + 3*t^5.07 + 3*t^5.17 + 3*t^5.43 + 3*t^5.53 + t^5.79 + 4*t^5.9 - t^6. + 2*t^6.26 + 2*t^6.36 + t^6.57 + t^6.62 + t^6.67 + t^6.72 + 2*t^6.83 + t^6.93 + t^7.04 + t^7.09 + 4*t^7.19 + 3*t^7.29 + 2*t^7.4 + t^7.45 + 4*t^7.55 + 6*t^7.65 + 2*t^7.76 + 3*t^7.91 + 6*t^8.02 + 2*t^8.12 - 4*t^8.22 + t^8.27 + 6*t^8.38 + 2*t^8.48 - 3*t^8.59 - t^8.69 + 3*t^8.74 + t^8.79 + 6*t^8.84 + t^8.9 - 5*t^8.95 - t^4.29/y - t^6.52/y - t^6.78/y - t^6.88/y - t^7.24/y + (2*t^7.35)/y + t^7.6/y + (3*t^7.71)/y + (2*t^7.81)/y + (4*t^8.07)/y + (2*t^8.17)/y + (3*t^8.43)/y + (4*t^8.53)/y + t^8.64/y - t^8.74/y + t^8.79/y + (3*t^8.9)/y - t^4.29*y - t^6.52*y - t^6.78*y - t^6.88*y - t^7.24*y + 2*t^7.35*y + t^7.6*y + 3*t^7.71*y + 2*t^7.81*y + 4*t^8.07*y + 2*t^8.17*y + 3*t^8.43*y + 4*t^8.53*y + t^8.64*y - t^8.74*y + t^8.79*y + 3*t^8.9*y | g1^6*t^2.12 + t^2.22/g1^22 + g1^24*t^2.48 + t^2.59/g1^4 + 2*g1^14*t^2.95 + g1^32*t^3.31 + g1^4*t^3.41 + t^3.88/g1^6 + g1^12*t^4.24 + t^4.35/g1^16 + t^4.45/g1^44 + g1^30*t^4.6 + 3*g1^2*t^4.71 + t^4.81/g1^26 + g1^48*t^4.96 + 3*g1^20*t^5.07 + (3*t^5.17)/g1^8 + 3*g1^38*t^5.43 + 3*g1^10*t^5.53 + g1^56*t^5.79 + 4*g1^28*t^5.9 - t^6. + 2*g1^46*t^6.26 + 2*g1^18*t^6.36 + t^6.57/g1^38 + g1^64*t^6.62 + t^6.67/g1^66 + g1^36*t^6.72 + 2*g1^8*t^6.83 + t^6.93/g1^20 + t^7.04/g1^48 + g1^54*t^7.09 + 4*g1^26*t^7.19 + (3*t^7.29)/g1^2 + (2*t^7.4)/g1^30 + g1^72*t^7.45 + 4*g1^44*t^7.55 + 6*g1^16*t^7.65 + (2*t^7.76)/g1^12 + 3*g1^62*t^7.91 + 6*g1^34*t^8.02 + 2*g1^6*t^8.12 - (4*t^8.22)/g1^22 + g1^80*t^8.27 + 6*g1^52*t^8.38 + 2*g1^24*t^8.48 - (3*t^8.59)/g1^4 - t^8.69/g1^32 + 3*g1^70*t^8.74 + t^8.79/g1^60 + 6*g1^42*t^8.84 + t^8.9/g1^88 - 5*g1^14*t^8.95 - t^4.29/(g1^2*y) - t^6.52/(g1^24*y) - (g1^22*t^6.78)/y - t^6.88/(g1^6*y) - (g1^12*t^7.24)/y + (2*t^7.35)/(g1^16*y) + (g1^30*t^7.6)/y + (3*g1^2*t^7.71)/y + (2*t^7.81)/(g1^26*y) + (4*g1^20*t^8.07)/y + (2*t^8.17)/(g1^8*y) + (3*g1^38*t^8.43)/y + (4*g1^10*t^8.53)/y + t^8.64/(g1^18*y) - t^8.74/(g1^46*y) + (g1^56*t^8.79)/y + (3*g1^28*t^8.9)/y - (t^4.29*y)/g1^2 - (t^6.52*y)/g1^24 - g1^22*t^6.78*y - (t^6.88*y)/g1^6 - g1^12*t^7.24*y + (2*t^7.35*y)/g1^16 + g1^30*t^7.6*y + 3*g1^2*t^7.71*y + (2*t^7.81*y)/g1^26 + 4*g1^20*t^8.07*y + (2*t^8.17*y)/g1^8 + 3*g1^38*t^8.43*y + 4*g1^10*t^8.53*y + (t^8.64*y)/g1^18 - (t^8.74*y)/g1^46 + g1^56*t^8.79*y + 3*g1^28*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2103 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ M_1M_3$ + $ M_3M_6$ + $ \phi_1q_1\tilde{q}_2$ | 0.5827 | 0.7345 | 0.7934 | [X:[], M:[1.0027, 0.71, 0.9973, 0.7155, 1.2845, 1.0027], q:[0.6423, 0.355], qb:[0.3605, 0.9296], phi:[0.4282]] | t^2.13 + t^2.15 + t^2.57 + 2*t^3.01 + t^3.41 + t^3.43 + t^3.45 + t^3.85 + t^4.26 + t^4.28 + t^4.29 + t^4.7 + 2*t^4.72 + 3*t^5.14 + 2*t^5.15 + t^5.54 + t^5.56 + 3*t^5.58 + t^5.59 + t^5.98 - t^6. - t^4.28/y - t^4.28*y | detail |