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 |
|---|---|---|---|---|---|---|---|---|---|
| 5883 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_4M_6$ + $ M_3M_5$ + $ M_5M_7$ + $ \phi_1q_1\tilde{q}_2$ + $ M_8\phi_1\tilde{q}_1^2$ + $ M_6M_9$ | 0.6046 | 0.7777 | 0.7774 | [X:[], M:[0.7487, 1.1366, 0.9781, 0.7049, 1.0219, 1.2951, 0.9781, 0.8196, 0.7049], q:[0.9208, 0.3306], qb:[0.3743, 0.6475], phi:[0.4317]] | [X:[], M:[[22], [-4], [-14], [-6], [14], [6], [-14], [-24], [-6]], q:[[-5], [-17]], qb:[[11], [3]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_9$, $ M_1$, $ M_8$, $ M_3$, $ M_7$, $ \phi_1q_2^2$, $ M_2$, $ \phi_1q_2\tilde{q}_1$, $ M_4^2$, $ M_4M_9$, $ M_9^2$, $ \phi_1q_2\tilde{q}_2$, $ M_1M_4$, $ M_1M_9$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ M_4M_8$, $ M_8M_9$, $ M_1M_8$, $ q_1\tilde{q}_2$, $ M_8^2$, $ M_3M_4$, $ M_4M_7$, $ M_3M_9$, $ M_7M_9$, $ \phi_1q_1q_2$, $ M_1M_3$, $ M_1M_7$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ M_3M_8$, $ M_7M_8$, $ M_4\phi_1q_2^2$, $ M_9\phi_1q_2^2$, $ M_2M_4$, $ M_2M_9$, $ M_4\phi_1q_2\tilde{q}_1$, $ M_9\phi_1q_2\tilde{q}_1$, $ M_1M_2$, $ M_8\phi_1q_2^2$, $ M_3^2$, $ M_3M_7$, $ M_7^2$, $ M_2M_8$, $ M_8\phi_1q_2\tilde{q}_1$ | . | -3 | 2*t^2.11 + t^2.25 + t^2.46 + 2*t^2.93 + t^3.28 + 2*t^3.41 + 3*t^4.23 + 2*t^4.36 + t^4.49 + 2*t^4.57 + 2*t^4.7 + t^4.92 + 4*t^5.05 + 2*t^5.18 + 4*t^5.39 + 4*t^5.52 + t^5.66 + t^5.74 + 4*t^5.87 - 3*t^6. - t^6.13 + 2*t^6.21 + 6*t^6.34 + t^6.48 + t^6.56 + 2*t^6.61 + 4*t^6.69 + t^6.74 + 3*t^6.82 + 2*t^7.03 + 6*t^7.16 + t^7.3 + t^7.38 + t^7.43 + 7*t^7.51 + 8*t^7.64 + 4*t^7.85 + t^7.9 + 8*t^7.98 - 3*t^8.11 + t^8.2 - 6*t^8.25 + 8*t^8.33 - t^8.38 + 5*t^8.46 - t^8.59 + 4*t^8.67 + t^8.72 + 10*t^8.8 + 2*t^8.85 - 4*t^8.93 + t^8.98 - t^4.3/y - t^6.41/y - t^6.54/y - t^6.75/y + (3*t^7.36)/y + (2*t^7.57)/y + t^7.7/y + t^7.84/y + (5*t^8.05)/y + (3*t^8.18)/y + (4*t^8.39)/y + (4*t^8.52)/y + t^8.66/y + t^8.74/y - t^8.79/y + (2*t^8.87)/y - t^4.3*y - t^6.41*y - t^6.54*y - t^6.75*y + 3*t^7.36*y + 2*t^7.57*y + t^7.7*y + t^7.84*y + 5*t^8.05*y + 3*t^8.18*y + 4*t^8.39*y + 4*t^8.52*y + t^8.66*y + t^8.74*y - t^8.79*y + 2*t^8.87*y | (2*t^2.11)/g1^6 + g1^22*t^2.25 + t^2.46/g1^24 + (2*t^2.93)/g1^14 + t^3.28/g1^32 + (2*t^3.41)/g1^4 + (3*t^4.23)/g1^12 + 2*g1^16*t^4.36 + g1^44*t^4.49 + (2*t^4.57)/g1^30 + (2*t^4.7)/g1^2 + t^4.92/g1^48 + (4*t^5.05)/g1^20 + 2*g1^8*t^5.18 + (4*t^5.39)/g1^38 + (4*t^5.52)/g1^10 + g1^18*t^5.66 + t^5.74/g1^56 + (4*t^5.87)/g1^28 - 3*t^6. - g1^28*t^6.13 + (2*t^6.21)/g1^46 + (6*t^6.34)/g1^18 + g1^10*t^6.48 + t^6.56/g1^64 + 2*g1^38*t^6.61 + (4*t^6.69)/g1^36 + g1^66*t^6.74 + (3*t^6.82)/g1^8 + (2*t^7.03)/g1^54 + (6*t^7.16)/g1^26 + g1^2*t^7.3 + t^7.38/g1^72 + g1^30*t^7.43 + (7*t^7.51)/g1^44 + (8*t^7.64)/g1^16 + (4*t^7.85)/g1^62 + g1^40*t^7.9 + (8*t^7.98)/g1^34 - (3*t^8.11)/g1^6 + t^8.2/g1^80 - 6*g1^22*t^8.25 + (8*t^8.33)/g1^52 - g1^50*t^8.38 + (5*t^8.46)/g1^24 - g1^4*t^8.59 + (4*t^8.67)/g1^70 + g1^32*t^8.72 + (10*t^8.8)/g1^42 + 2*g1^60*t^8.85 - (4*t^8.93)/g1^14 + g1^88*t^8.98 - (g1^2*t^4.3)/y - t^6.41/(g1^4*y) - (g1^24*t^6.54)/y - t^6.75/(g1^22*y) + (3*g1^16*t^7.36)/y + (2*t^7.57)/(g1^30*y) + t^7.7/(g1^2*y) + (g1^26*t^7.84)/y + (5*t^8.05)/(g1^20*y) + (3*g1^8*t^8.18)/y + (4*t^8.39)/(g1^38*y) + (4*t^8.52)/(g1^10*y) + (g1^18*t^8.66)/y + t^8.74/(g1^56*y) - (g1^46*t^8.79)/y + (2*t^8.87)/(g1^28*y) - g1^2*t^4.3*y - (t^6.41*y)/g1^4 - g1^24*t^6.54*y - (t^6.75*y)/g1^22 + 3*g1^16*t^7.36*y + (2*t^7.57*y)/g1^30 + (t^7.7*y)/g1^2 + g1^26*t^7.84*y + (5*t^8.05*y)/g1^20 + 3*g1^8*t^8.18*y + (4*t^8.39*y)/g1^38 + (4*t^8.52*y)/g1^10 + g1^18*t^8.66*y + (t^8.74*y)/g1^56 - g1^46*t^8.79*y + (2*t^8.87*y)/g1^28 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4393 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_4M_6$ + $ M_3M_5$ + $ M_5M_7$ + $ \phi_1q_1\tilde{q}_2$ + $ M_8\phi_1\tilde{q}_1^2$ | 0.5841 | 0.7387 | 0.7908 | [X:[], M:[0.7467, 1.137, 0.9794, 0.7055, 1.0206, 1.2945, 0.9794, 0.8218], q:[0.9212, 0.3321], qb:[0.3733, 0.6473], phi:[0.4315]] | t^2.12 + t^2.24 + t^2.47 + 2*t^2.94 + t^3.29 + 2*t^3.41 + t^3.88 + t^4.23 + t^4.36 + t^4.48 + t^4.58 + 2*t^4.71 + t^4.93 + 2*t^5.05 + 2*t^5.18 + 3*t^5.4 + 2*t^5.53 + t^5.65 + t^5.75 + 4*t^5.88 - 2*t^6. - t^4.29/y - t^4.29*y | detail |