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 |
|---|---|---|---|---|---|---|---|---|---|
| 56203 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_4\phi_1q_1^2$ + $ M_6\phi_1q_1q_2$ + $ M_2M_7$ | 0.6874 | 0.8631 | 0.7964 | [X:[], M:[1.1604, 1.0375, 0.8396, 0.7736, 0.9715, 0.7077, 0.9625], q:[0.3868, 0.4528], qb:[0.5757, 0.7736], phi:[0.4528]] | [X:[], M:[[3], [-18], [-3], [2], [-13], [7], [18]], q:[[1], [-4]], qb:[[17], [2]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_6$, $ M_4$, $ M_3$, $ \phi_1^2$, $ M_7$, $ M_5$, $ M_1$, $ \phi_1q_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_4^2$, $ M_3M_6$, $ \phi_1\tilde{q}_1^2$, $ M_3M_4$, $ M_6\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_6M_7$, $ M_3^2$, $ M_5M_6$, $ M_4\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_4M_7$, $ M_4M_5$, $ M_3\phi_1^2$, $ M_3M_7$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3M_5$, $ \phi_1^4$, $ M_1M_6$, $ M_7\phi_1^2$, $ M_7^2$, $ M_1M_4$, $ M_5M_7$, $ M_6\phi_1q_1^2$, $ M_5^2$ | . | -1 | t^2.12 + t^2.32 + t^2.52 + t^2.72 + t^2.89 + t^2.91 + t^3.48 + t^3.68 + t^4.05 + t^4.07 + 2*t^4.25 + 2*t^4.44 + 2*t^4.64 + t^4.81 + 2*t^4.84 + t^5.01 + 3*t^5.04 + t^5.21 + 2*t^5.24 + t^5.41 + t^5.43 + 2*t^5.6 + t^5.78 + 2*t^5.8 + t^5.83 - t^6. + t^6.17 + t^6.2 + 3*t^6.37 + 2*t^6.4 + 3*t^6.57 + t^6.59 + 3*t^6.76 + 2*t^6.94 + 5*t^6.96 + 3*t^7.13 + 4*t^7.16 + 2*t^7.33 + 2*t^7.36 + 3*t^7.53 + 3*t^7.56 + t^7.7 + 3*t^7.73 + 2*t^7.75 + t^7.9 + 3*t^7.93 + 2*t^7.95 + t^8.1 + 2*t^8.15 + 3*t^8.29 - t^8.32 + 5*t^8.49 + t^8.55 + t^8.66 + 3*t^8.69 + t^8.74 + t^8.86 + 2*t^8.89 - 2*t^8.91 - t^4.36/y - t^6.48/y - t^6.68/y - t^7.07/y - t^7.27/y + (2*t^7.44)/y + (2*t^7.64)/y + (2*t^7.84)/y + t^8.01/y + (3*t^8.04)/y + t^8.21/y + (3*t^8.24)/y + t^8.41/y + t^8.43/y + t^8.6/y + t^8.63/y + (2*t^8.8)/y - t^4.36*y - t^6.48*y - t^6.68*y - t^7.07*y - t^7.27*y + 2*t^7.44*y + 2*t^7.64*y + 2*t^7.84*y + t^8.01*y + 3*t^8.04*y + t^8.21*y + 3*t^8.24*y + t^8.41*y + t^8.43*y + t^8.6*y + t^8.63*y + 2*t^8.8*y | g1^7*t^2.12 + g1^2*t^2.32 + t^2.52/g1^3 + t^2.72/g1^8 + g1^18*t^2.89 + t^2.91/g1^13 + g1^3*t^3.48 + t^3.68/g1^2 + g1^19*t^4.05 + t^4.07/g1^12 + 2*g1^14*t^4.25 + 2*g1^9*t^4.44 + 2*g1^4*t^4.64 + g1^30*t^4.81 + (2*t^4.84)/g1 + g1^25*t^5.01 + (3*t^5.04)/g1^6 + g1^20*t^5.21 + (2*t^5.24)/g1^11 + g1^15*t^5.41 + t^5.43/g1^16 + 2*g1^10*t^5.6 + g1^36*t^5.78 + 2*g1^5*t^5.8 + t^5.83/g1^26 - t^6. + g1^26*t^6.17 + t^6.2/g1^5 + 3*g1^21*t^6.37 + (2*t^6.4)/g1^10 + 3*g1^16*t^6.57 + t^6.59/g1^15 + 3*g1^11*t^6.76 + 2*g1^37*t^6.94 + 5*g1^6*t^6.96 + 3*g1^32*t^7.13 + 4*g1*t^7.16 + 2*g1^27*t^7.33 + (2*t^7.36)/g1^4 + 3*g1^22*t^7.53 + (3*t^7.56)/g1^9 + g1^48*t^7.7 + 3*g1^17*t^7.73 + (2*t^7.75)/g1^14 + g1^43*t^7.9 + 3*g1^12*t^7.93 + (2*t^7.95)/g1^19 + g1^38*t^8.1 + (2*t^8.15)/g1^24 + 3*g1^33*t^8.29 - g1^2*t^8.32 + 5*g1^28*t^8.49 + t^8.55/g1^34 + g1^54*t^8.66 + 3*g1^23*t^8.69 + t^8.74/g1^39 + g1^49*t^8.86 + 2*g1^18*t^8.89 - (2*t^8.91)/g1^13 - t^4.36/(g1^4*y) - (g1^3*t^6.48)/y - t^6.68/(g1^2*y) - t^7.07/(g1^12*y) - t^7.27/(g1^17*y) + (2*g1^9*t^7.44)/y + (2*g1^4*t^7.64)/y + (2*t^7.84)/(g1*y) + (g1^25*t^8.01)/y + (3*t^8.04)/(g1^6*y) + (g1^20*t^8.21)/y + (3*t^8.24)/(g1^11*y) + (g1^15*t^8.41)/y + t^8.43/(g1^16*y) + (g1^10*t^8.6)/y + t^8.63/(g1^21*y) + (2*g1^5*t^8.8)/y - (t^4.36*y)/g1^4 - g1^3*t^6.48*y - (t^6.68*y)/g1^2 - (t^7.07*y)/g1^12 - (t^7.27*y)/g1^17 + 2*g1^9*t^7.44*y + 2*g1^4*t^7.64*y + (2*t^7.84*y)/g1 + g1^25*t^8.01*y + (3*t^8.04*y)/g1^6 + g1^20*t^8.21*y + (3*t^8.24*y)/g1^11 + g1^15*t^8.41*y + (t^8.43*y)/g1^16 + g1^10*t^8.6*y + (t^8.63*y)/g1^21 + 2*g1^5*t^8.8*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50984 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_4\phi_1q_1^2$ + $ M_6\phi_1q_1q_2$ | 0.6866 | 0.8604 | 0.798 | [X:[], M:[1.1704, 0.9776, 0.8296, 0.7803, 0.9283, 0.7309], q:[0.3901, 0.4395], qb:[0.6323, 0.7803], phi:[0.4395]] | t^2.19 + t^2.34 + t^2.49 + t^2.64 + t^2.78 + t^2.93 + t^3.51 + t^3.66 + t^3.96 + t^4.24 + 2*t^4.39 + 2*t^4.53 + 2*t^4.68 + 2*t^4.83 + 3*t^4.98 + t^5.11 + 3*t^5.13 + 2*t^5.27 + t^5.42 + 2*t^5.57 + t^5.7 + t^5.72 + t^5.85 + t^5.87 - t^6. - t^4.32/y - t^4.32*y | detail |