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 |
|---|---|---|---|---|---|---|---|---|---|
| 4102 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_1M_4$ + $ M_5q_1\tilde{q}_1$ + $ M_6q_1q_2$ + $ M_1M_5$ + $ M_7\phi_1q_2^2$ + $ M_1M_8$ | 0.6691 | 0.8502 | 0.787 | [X:[], M:[1.1775, 1.215, 0.7475, 0.8225, 0.8225, 0.7475, 0.71, 0.8225], q:[0.8037, 0.4487], qb:[0.3738, 0.8037], phi:[0.3925]] | [X:[], M:[[-6], [4], [-14], [6], [6], [-14], [-24], [6]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_7$, $ M_3$, $ M_6$, $ M_4$, $ M_5$, $ M_8$, $ \phi_1\tilde{q}_1^2$, $ M_2$, $ \phi_1q_2\tilde{q}_1$, $ M_7^2$, $ M_3M_7$, $ M_6M_7$, $ M_3^2$, $ M_3M_6$, $ M_6^2$, $ M_4M_7$, $ M_5M_7$, $ M_7M_8$, $ M_3M_4$, $ M_3M_5$, $ M_4M_6$, $ M_5M_6$, $ M_3M_8$, $ M_6M_8$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_2$, $ M_4^2$, $ M_4M_5$, $ M_5^2$, $ M_4M_8$, $ M_5M_8$, $ M_8^2$, $ \phi_1q_2\tilde{q}_2$, $ M_7\phi_1\tilde{q}_1^2$, $ M_3\phi_1\tilde{q}_1^2$, $ M_6\phi_1\tilde{q}_1^2$, $ M_2M_7$, $ M_7\phi_1q_2\tilde{q}_1$, $ M_2M_3$, $ M_2M_6$, $ M_6\phi_1q_2\tilde{q}_1$, $ M_4\phi_1\tilde{q}_1^2$, $ M_5\phi_1\tilde{q}_1^2$, $ M_8\phi_1\tilde{q}_1^2$ | $\phi_1\tilde{q}_2^2$ | -3 | t^2.13 + 2*t^2.24 + 3*t^2.47 + t^3.42 + 2*t^3.64 + t^4.26 + 2*t^4.37 + 3*t^4.49 + 3*t^4.6 + 6*t^4.71 + t^4.82 + 6*t^4.93 + t^5.55 + 2*t^5.66 + t^5.78 + 5*t^5.89 - 3*t^6. + 4*t^6.11 - t^6.22 + t^6.39 + 2*t^6.5 + 3*t^6.62 + 7*t^6.73 + 7*t^6.84 + 9*t^6.95 + 7*t^7.07 + 8*t^7.18 + t^7.29 + 7*t^7.4 - t^7.51 + t^7.68 + 2*t^7.79 + 4*t^7.91 + 3*t^8.02 + 5*t^8.13 - 5*t^8.24 + 6*t^8.36 - 11*t^8.47 + t^8.52 + 4*t^8.58 + 2*t^8.63 - 4*t^8.69 + 3*t^8.75 + 7*t^8.86 + 12*t^8.97 - t^4.18/y - t^6.31/y - (2*t^6.42)/y - (2*t^6.64)/y + (2*t^7.37)/y + t^7.49/y + (3*t^7.6)/y + (8*t^7.71)/y + (5*t^7.93)/y + t^8.05/y - t^8.44/y - t^8.55/y - t^8.66/y + (3*t^8.89)/y - t^4.18*y - t^6.31*y - 2*t^6.42*y - 2*t^6.64*y + 2*t^7.37*y + t^7.49*y + 3*t^7.6*y + 8*t^7.71*y + 5*t^7.93*y + t^8.05*y - t^8.44*y - t^8.55*y - t^8.66*y + 3*t^8.89*y | t^2.13/g1^24 + (2*t^2.24)/g1^14 + 3*g1^6*t^2.47 + t^3.42/g1^16 + 2*g1^4*t^3.64 + t^4.26/g1^48 + (2*t^4.37)/g1^38 + (3*t^4.49)/g1^28 + (3*t^4.6)/g1^18 + (6*t^4.71)/g1^8 + g1^2*t^4.82 + 6*g1^12*t^4.93 + t^5.55/g1^40 + (2*t^5.66)/g1^30 + t^5.78/g1^20 + (5*t^5.89)/g1^10 - 3*t^6. + 4*g1^10*t^6.11 - g1^20*t^6.22 + t^6.39/g1^72 + (2*t^6.5)/g1^62 + (3*t^6.62)/g1^52 + (7*t^6.73)/g1^42 + (7*t^6.84)/g1^32 + (9*t^6.95)/g1^22 + (7*t^7.07)/g1^12 + (8*t^7.18)/g1^2 + g1^8*t^7.29 + 7*g1^18*t^7.4 - g1^28*t^7.51 + t^7.68/g1^64 + (2*t^7.79)/g1^54 + (4*t^7.91)/g1^44 + (3*t^8.02)/g1^34 + (5*t^8.13)/g1^24 - (5*t^8.24)/g1^14 + (6*t^8.36)/g1^4 - 11*g1^6*t^8.47 + t^8.52/g1^96 + 4*g1^16*t^8.58 + (2*t^8.63)/g1^86 - 4*g1^26*t^8.69 + (3*t^8.75)/g1^76 + (7*t^8.86)/g1^66 + (12*t^8.97)/g1^56 - t^4.18/(g1^2*y) - t^6.31/(g1^26*y) - (2*t^6.42)/(g1^16*y) - (2*g1^4*t^6.64)/y + (2*t^7.37)/(g1^38*y) + t^7.49/(g1^28*y) + (3*t^7.6)/(g1^18*y) + (8*t^7.71)/(g1^8*y) + (5*g1^12*t^7.93)/y + (g1^22*t^8.05)/y - t^8.44/(g1^50*y) - t^8.55/(g1^40*y) - t^8.66/(g1^30*y) + (3*t^8.89)/(g1^10*y) - (t^4.18*y)/g1^2 - (t^6.31*y)/g1^26 - (2*t^6.42*y)/g1^16 - 2*g1^4*t^6.64*y + (2*t^7.37*y)/g1^38 + (t^7.49*y)/g1^28 + (3*t^7.6*y)/g1^18 + (8*t^7.71*y)/g1^8 + 5*g1^12*t^7.93*y + g1^22*t^8.05*y - (t^8.44*y)/g1^50 - (t^8.55*y)/g1^40 - (t^8.66*y)/g1^30 + (3*t^8.89*y)/g1^10 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2118 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_1M_4$ + $ M_5q_1\tilde{q}_1$ + $ M_6q_1q_2$ + $ M_1M_5$ + $ M_7\phi_1q_2^2$ | 0.6541 | 0.825 | 0.7928 | [X:[], M:[1.1748, 1.2168, 0.7412, 0.8252, 0.8252, 0.7412, 0.6992], q:[0.8042, 0.4546], qb:[0.3706, 0.8042], phi:[0.3916]] | t^2.1 + 2*t^2.22 + 2*t^2.48 + t^3.4 + t^3.52 + 2*t^3.65 + t^4.2 + 2*t^4.32 + 3*t^4.45 + 2*t^4.57 + 4*t^4.7 + t^4.83 + 3*t^4.95 + t^5.5 + 3*t^5.62 + 3*t^5.75 + 4*t^5.87 - t^6. - t^4.17/y - t^4.17*y | detail |