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 |
|---|---|---|---|---|---|---|---|---|---|
| 55923 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1q_1^2$ + $ M_2M_5$ + $ M_1M_6$ | 0.6697 | 0.84 | 0.7972 | [X:[], M:[1.1151, 1.1506, 0.8849, 0.6904, 0.8494, 0.8849], q:[0.3452, 0.5398], qb:[0.5042, 0.7699], phi:[0.4602]] | [X:[], M:[[-1], [-10], [1], [-6], [10], [1]], q:[[-3], [4]], qb:[[13], [2]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_5$, $ M_3$, $ M_6$, $ \phi_1^2$, $ q_2\tilde{q}_1$, $ M_2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1q_2$, $ M_4^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_1$, $ M_4M_5$, $ \phi_1q_2^2$, $ M_3M_4$, $ M_4M_6$, $ \phi_1q_1\tilde{q}_2$, $ M_4\phi_1^2$, $ M_5^2$, $ M_3M_5$, $ M_5M_6$, $ M_4q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ M_3M_6$, $ M_6^2$, $ M_5\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_3\phi_1^2$, $ M_6\phi_1^2$, $ M_2M_4$, $ \phi_1^4$, $ M_5q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_4\tilde{q}_1\tilde{q}_2$ | $M_4\phi_1q_1\tilde{q}_1$ | -1 | t^2.07 + t^2.55 + 2*t^2.65 + t^2.76 + t^3.13 + t^3.45 + t^3.82 + t^3.93 + t^4.04 + t^4.14 + t^4.41 + t^4.51 + 2*t^4.62 + 2*t^4.73 + t^4.83 + t^5.1 + 3*t^5.2 + 4*t^5.31 + t^5.42 + t^5.52 + t^5.68 + 2*t^5.79 + t^5.89 - t^6. + t^6.11 + 2*t^6.21 + t^6.26 + t^6.37 + 2*t^6.48 + 3*t^6.58 + 2*t^6.69 + t^6.8 + t^6.9 + 2*t^6.95 + 3*t^7.06 + 4*t^7.17 + 3*t^7.27 + 3*t^7.38 + t^7.49 + t^7.54 + t^7.59 + 2*t^7.64 + 3*t^7.75 + 4*t^7.86 + 4*t^7.96 + t^8.07 + 2*t^8.23 + 2*t^8.28 + 4*t^8.33 + 4*t^8.44 - t^8.55 - 3*t^8.65 + 2*t^8.81 + t^8.87 + 4*t^8.92 + 2*t^8.97 - t^4.38/y - t^6.45/y - t^7.04/y - t^7.14/y + (2*t^7.62)/y + (3*t^7.73)/y + t^7.83/y + (3*t^8.2)/y + (3*t^8.31)/y + (2*t^8.42)/y + t^8.68/y + (2*t^8.79)/y + (2*t^8.89)/y - t^4.38*y - t^6.45*y - t^7.04*y - t^7.14*y + 2*t^7.62*y + 3*t^7.73*y + t^7.83*y + 3*t^8.2*y + 3*t^8.31*y + 2*t^8.42*y + t^8.68*y + 2*t^8.79*y + 2*t^8.89*y | t^2.07/g1^6 + g1^10*t^2.55 + 2*g1*t^2.65 + t^2.76/g1^8 + g1^17*t^3.13 + t^3.45/g1^10 + g1^15*t^3.82 + g1^6*t^3.93 + t^4.04/g1^3 + t^4.14/g1^12 + g1^22*t^4.41 + g1^13*t^4.51 + 2*g1^4*t^4.62 + (2*t^4.73)/g1^5 + t^4.83/g1^14 + g1^20*t^5.1 + 3*g1^11*t^5.2 + 4*g1^2*t^5.31 + t^5.42/g1^7 + t^5.52/g1^16 + g1^27*t^5.68 + 2*g1^18*t^5.79 + g1^9*t^5.89 - t^6. + t^6.11/g1^9 + (2*t^6.21)/g1^18 + g1^34*t^6.26 + g1^25*t^6.37 + 2*g1^16*t^6.48 + 3*g1^7*t^6.58 + (2*t^6.69)/g1^2 + t^6.8/g1^11 + t^6.9/g1^20 + 2*g1^32*t^6.95 + 3*g1^23*t^7.06 + 4*g1^14*t^7.17 + 3*g1^5*t^7.27 + (3*t^7.38)/g1^4 + t^7.49/g1^13 + g1^39*t^7.54 + t^7.59/g1^22 + 2*g1^30*t^7.64 + 3*g1^21*t^7.75 + 4*g1^12*t^7.86 + 4*g1^3*t^7.96 + t^8.07/g1^6 + 2*g1^37*t^8.23 + (2*t^8.28)/g1^24 + 4*g1^28*t^8.33 + 4*g1^19*t^8.44 - g1^10*t^8.55 - 3*g1*t^8.65 + 2*g1^44*t^8.81 + t^8.87/g1^17 + 4*g1^35*t^8.92 + (2*t^8.97)/g1^26 - t^4.38/(g1^4*y) - t^6.45/(g1^10*y) - t^7.04/(g1^3*y) - t^7.14/(g1^12*y) + (2*g1^4*t^7.62)/y + (3*t^7.73)/(g1^5*y) + t^7.83/(g1^14*y) + (3*g1^11*t^8.2)/y + (3*g1^2*t^8.31)/y + (2*t^8.42)/(g1^7*y) + (g1^27*t^8.68)/y + (2*g1^18*t^8.79)/y + (2*g1^9*t^8.89)/y - (t^4.38*y)/g1^4 - (t^6.45*y)/g1^10 - (t^7.04*y)/g1^3 - (t^7.14*y)/g1^12 + 2*g1^4*t^7.62*y + (3*t^7.73*y)/g1^5 + (t^7.83*y)/g1^14 + 3*g1^11*t^8.2*y + 3*g1^2*t^8.31*y + (2*t^8.42*y)/g1^7 + g1^27*t^8.68*y + 2*g1^18*t^8.79*y + 2*g1^9*t^8.89*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 |
|---|---|---|---|---|---|---|---|---|---|
| 48173 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1q_1^2$ + $ M_2M_5$ | 0.6593 | 0.8223 | 0.8018 | [X:[], M:[1.1149, 1.1485, 0.8851, 0.6891, 0.8515], q:[0.3446, 0.5406], qb:[0.5069, 0.7703], phi:[0.4594]] | t^2.07 + t^2.55 + t^2.66 + t^2.76 + t^3.14 + t^3.34 + t^3.45 + t^3.83 + t^3.93 + t^4.03 + t^4.13 + t^4.42 + t^4.52 + 2*t^4.62 + t^4.72 + t^4.82 + t^5.11 + 2*t^5.21 + 2*t^5.31 + t^5.41 + t^5.51 + t^5.7 + t^5.8 + 2*t^5.9 - t^4.38/y - t^4.38*y | detail |