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 |
|---|---|---|---|---|---|---|---|---|---|
| 4877 | 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_1M_6$ + $ M_7\phi_1q_2^2$ + $ \phi_1q_1\tilde{q}_2$ + $ M_8\phi_1q_2\tilde{q}_1$ | 0.6085 | 0.7786 | 0.7816 | [X:[], M:[1.0144, 0.6917, 0.9856, 0.7204, 1.2796, 0.9856, 0.8818, 0.853], q:[0.6398, 0.3459], qb:[0.3746, 0.9337], phi:[0.4265]] | [X:[], M:[[14], [-22], [-14], [6], [-6], [-14], [24], [-4]], q:[[-3], [-11]], qb:[[17], [5]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ M_4$, $ M_8$, $ \phi_1^2$, $ M_7$, $ M_3$, $ M_6$, $ \phi_1\tilde{q}_1^2$, $ M_5$, $ M_2^2$, $ M_2M_4$, $ \phi_1q_1q_2$, $ M_4^2$, $ \phi_1q_1\tilde{q}_1$, $ M_2M_8$, $ M_2\phi_1^2$, $ M_2M_7$, $ M_4M_8$, $ M_4\phi_1^2$, $ q_1\tilde{q}_2$, $ M_4M_7$, $ M_2M_3$, $ M_2M_6$, $ M_3M_4$, $ M_4M_6$, $ M_8^2$, $ M_8\phi_1^2$, $ \phi_1^4$, $ \phi_1q_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_7M_8$, $ M_7\phi_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_7^2$, $ M_3M_8$, $ M_6M_8$, $ M_3\phi_1^2$, $ M_6\phi_1^2$, $ M_3M_7$, $ M_6M_7$, $ M_4\phi_1\tilde{q}_1^2$, $ M_3^2$, $ M_2M_5$, $ M_3M_6$, $ M_6^2$ | . | -2 | t^2.08 + t^2.16 + 2*t^2.56 + t^2.65 + 2*t^2.96 + t^3.53 + t^3.84 + t^4.15 + t^4.24 + t^4.32 + 2*t^4.63 + 4*t^4.72 + t^4.81 + 2*t^5.03 + 5*t^5.12 + 2*t^5.2 + t^5.29 + 3*t^5.52 + 2*t^5.6 + t^5.69 + 3*t^5.91 - 2*t^6. + t^6.09 + t^6.17 + t^6.23 + t^6.31 + t^6.4 + 2*t^6.48 + 2*t^6.71 + 4*t^6.8 + t^7.05 + 2*t^7.11 + 4*t^7.19 + 6*t^7.28 + 3*t^7.37 + t^7.45 + 3*t^7.59 + 10*t^7.68 + 3*t^7.76 + 3*t^7.85 + t^7.94 + 3*t^7.99 + 3*t^8.08 - 2*t^8.16 + 3*t^8.25 + t^8.3 + t^8.33 + t^8.39 + 3*t^8.47 - 3*t^8.56 - t^8.65 + t^8.73 + 2*t^8.78 + t^8.82 + 6*t^8.87 - 5*t^8.96 - t^4.28/y - t^6.35/y - (2*t^6.84)/y - t^6.92/y + t^7.32/y + (3*t^7.63)/y + (5*t^7.72)/y + t^7.81/y + (2*t^8.03)/y + (3*t^8.12)/y + (3*t^8.2)/y - t^8.43/y + (4*t^8.52)/y + (3*t^8.6)/y + t^8.69/y - t^4.28*y - t^6.35*y - 2*t^6.84*y - t^6.92*y + t^7.32*y + 3*t^7.63*y + 5*t^7.72*y + t^7.81*y + 2*t^8.03*y + 3*t^8.12*y + 3*t^8.2*y - t^8.43*y + 4*t^8.52*y + 3*t^8.6*y + t^8.69*y | t^2.08/g1^22 + g1^6*t^2.16 + (2*t^2.56)/g1^4 + g1^24*t^2.65 + (2*t^2.96)/g1^14 + g1^32*t^3.53 + t^3.84/g1^6 + t^4.15/g1^44 + t^4.24/g1^16 + g1^12*t^4.32 + (2*t^4.63)/g1^26 + 4*g1^2*t^4.72 + g1^30*t^4.81 + (2*t^5.03)/g1^36 + (5*t^5.12)/g1^8 + 2*g1^20*t^5.2 + g1^48*t^5.29 + (3*t^5.52)/g1^18 + 2*g1^10*t^5.6 + g1^38*t^5.69 + (3*t^5.91)/g1^28 - 2*t^6. + g1^28*t^6.09 + g1^56*t^6.17 + t^6.23/g1^66 + t^6.31/g1^38 + t^6.4/g1^10 + 2*g1^18*t^6.48 + (2*t^6.71)/g1^48 + (4*t^6.8)/g1^20 + g1^64*t^7.05 + (2*t^7.11)/g1^58 + (4*t^7.19)/g1^30 + (6*t^7.28)/g1^2 + 3*g1^26*t^7.37 + g1^54*t^7.45 + (3*t^7.59)/g1^40 + (10*t^7.68)/g1^12 + 3*g1^16*t^7.76 + 3*g1^44*t^7.85 + g1^72*t^7.94 + (3*t^7.99)/g1^50 + (3*t^8.08)/g1^22 - 2*g1^6*t^8.16 + 3*g1^34*t^8.25 + t^8.3/g1^88 + g1^62*t^8.33 + t^8.39/g1^60 + (3*t^8.47)/g1^32 - (3*t^8.56)/g1^4 - g1^24*t^8.65 + g1^52*t^8.73 + (2*t^8.78)/g1^70 + g1^80*t^8.82 + (6*t^8.87)/g1^42 - (5*t^8.96)/g1^14 - t^4.28/(g1^2*y) - t^6.35/(g1^24*y) - (2*t^6.84)/(g1^6*y) - (g1^22*t^6.92)/y + (g1^12*t^7.32)/y + (3*t^7.63)/(g1^26*y) + (5*g1^2*t^7.72)/y + (g1^30*t^7.81)/y + (2*t^8.03)/(g1^36*y) + (3*t^8.12)/(g1^8*y) + (3*g1^20*t^8.2)/y - t^8.43/(g1^46*y) + (4*t^8.52)/(g1^18*y) + (3*g1^10*t^8.6)/y + (g1^38*t^8.69)/y - (t^4.28*y)/g1^2 - (t^6.35*y)/g1^24 - (2*t^6.84*y)/g1^6 - g1^22*t^6.92*y + g1^12*t^7.32*y + (3*t^7.63*y)/g1^26 + 5*g1^2*t^7.72*y + g1^30*t^7.81*y + (2*t^8.03*y)/g1^36 + (3*t^8.12*y)/g1^8 + 3*g1^20*t^8.2*y - (t^8.43*y)/g1^46 + (4*t^8.52*y)/g1^18 + 3*g1^10*t^8.6*y + g1^38*t^8.69*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2702 | 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_1M_6$ + $ M_7\phi_1q_2^2$ + $ \phi_1q_1\tilde{q}_2$ | 0.5957 | 0.7565 | 0.7874 | [X:[], M:[1.011, 0.6969, 0.989, 0.719, 1.281, 0.989, 0.8761], q:[0.6405, 0.3485], qb:[0.3706, 0.9325], phi:[0.427]] | t^2.09 + t^2.16 + t^2.56 + t^2.63 + 2*t^2.97 + t^3.44 + t^3.5 + t^3.84 + t^4.18 + t^4.25 + t^4.31 + t^4.65 + 3*t^4.72 + t^4.79 + 2*t^5.06 + 3*t^5.12 + t^5.19 + t^5.26 + 2*t^5.53 + 3*t^5.6 + t^5.66 + 3*t^5.93 - t^6. - t^4.28/y - t^4.28*y | detail |