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 |
|---|---|---|---|---|---|---|---|---|---|
| 55640 | 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_2\phi_1^2$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1q_1q_2$ + $ M_6\tilde{q}_1\tilde{q}_2$ | 0.6997 | 0.8922 | 0.7843 | [X:[], M:[1.1503, 1.0797, 0.8497, 0.7608, 0.6902, 0.6902], q:[0.3804, 0.4693], qb:[0.5399, 0.7699], phi:[0.4601]] | [X:[], M:[[-5], [4], [5], [-12], [-3], [-3]], q:[[-6], [11]], qb:[[2], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ M_6$, $ M_4$, $ M_3$, $ \phi_1^2$, $ q_2\tilde{q}_1$, $ M_2$, $ M_1$, $ \phi_1q_1^2$, $ M_5^2$, $ M_5M_6$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_2^2$, $ M_4M_5$, $ M_4M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_4^2$, $ M_3M_5$, $ M_3M_6$, $ \phi_1\tilde{q}_1^2$, $ M_3M_4$, $ M_5\phi_1^2$, $ M_6\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_4\phi_1^2$, $ M_3^2$, $ M_5q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ M_2M_5$, $ M_2M_6$, $ M_3\phi_1^2$, $ M_4q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2M_4$, $ M_1M_5$, $ M_1M_6$, $ \phi_1^4$, $ M_3q_2\tilde{q}_1$, $ M_1M_4$, $ M_5\phi_1q_1^2$, $ M_6\phi_1q_1^2$, $ M_2M_3$, $ \phi_1^2q_2\tilde{q}_1$, $ M_4\phi_1q_1^2$ | . | -1 | 2*t^2.07 + t^2.28 + t^2.55 + t^2.76 + t^3.03 + t^3.24 + t^3.45 + t^3.66 + 4*t^4.14 + t^4.2 + 2*t^4.35 + t^4.41 + t^4.56 + 3*t^4.62 + 3*t^4.83 + t^5.04 + 3*t^5.1 + 4*t^5.31 + 3*t^5.52 + t^5.58 + 2*t^5.73 + t^5.79 + t^5.94 - t^6. + t^6.06 + 6*t^6.21 + 2*t^6.27 + 5*t^6.42 + 2*t^6.48 + 2*t^6.64 + 6*t^6.69 + t^6.75 + t^6.85 + 6*t^6.9 + t^6.96 + 3*t^7.11 + 4*t^7.17 + t^7.22 + 2*t^7.33 + 6*t^7.38 + t^7.44 + 6*t^7.59 + 3*t^7.65 + 5*t^7.8 + 2*t^7.86 + 2*t^8.02 - 2*t^8.07 + 2*t^8.13 + t^8.23 + 7*t^8.28 + 3*t^8.34 + t^8.39 + 7*t^8.49 + 2*t^8.6 + 5*t^8.71 + 7*t^8.76 + 3*t^8.82 + 2*t^8.92 + 9*t^8.97 - t^4.38/y - (2*t^6.45)/y - t^6.66/y + t^7.14/y + (2*t^7.35)/y + (2*t^7.62)/y + (3*t^7.83)/y + t^8.04/y + (3*t^8.1)/y + (6*t^8.31)/y + t^8.58/y + t^8.73/y + (2*t^8.79)/y - t^4.38*y - 2*t^6.45*y - t^6.66*y + t^7.14*y + 2*t^7.35*y + 2*t^7.62*y + 3*t^7.83*y + t^8.04*y + 3*t^8.1*y + 6*t^8.31*y + t^8.58*y + t^8.73*y + 2*t^8.79*y | (2*t^2.07)/g1^3 + t^2.28/g1^12 + g1^5*t^2.55 + t^2.76/g1^4 + g1^13*t^3.03 + g1^4*t^3.24 + t^3.45/g1^5 + t^3.66/g1^14 + (4*t^4.14)/g1^6 + g1^20*t^4.2 + (2*t^4.35)/g1^15 + g1^11*t^4.41 + t^4.56/g1^24 + 3*g1^2*t^4.62 + (3*t^4.83)/g1^7 + t^5.04/g1^16 + 3*g1^10*t^5.1 + 4*g1*t^5.31 + (3*t^5.52)/g1^8 + g1^18*t^5.58 + (2*t^5.73)/g1^17 + g1^9*t^5.79 + t^5.94/g1^26 - t^6. + g1^26*t^6.06 + (6*t^6.21)/g1^9 + 2*g1^17*t^6.27 + (5*t^6.42)/g1^18 + 2*g1^8*t^6.48 + (2*t^6.64)/g1^27 + (6*t^6.69)/g1 + g1^25*t^6.75 + t^6.85/g1^36 + (6*t^6.9)/g1^10 + g1^16*t^6.96 + (3*t^7.11)/g1^19 + 4*g1^7*t^7.17 + g1^33*t^7.22 + (2*t^7.33)/g1^28 + (6*t^7.38)/g1^2 + g1^24*t^7.44 + (6*t^7.59)/g1^11 + 3*g1^15*t^7.65 + (5*t^7.8)/g1^20 + 2*g1^6*t^7.86 + (2*t^8.02)/g1^29 - (2*t^8.07)/g1^3 + 2*g1^23*t^8.13 + t^8.23/g1^38 + (7*t^8.28)/g1^12 + 3*g1^14*t^8.34 + g1^40*t^8.39 + (7*t^8.49)/g1^21 + 2*g1^31*t^8.6 + (5*t^8.71)/g1^30 + (7*t^8.76)/g1^4 + 3*g1^22*t^8.82 + (2*t^8.92)/g1^39 + (9*t^8.97)/g1^13 - t^4.38/(g1^2*y) - (2*t^6.45)/(g1^5*y) - t^6.66/(g1^14*y) + t^7.14/(g1^6*y) + (2*t^7.35)/(g1^15*y) + (2*g1^2*t^7.62)/y + (3*t^7.83)/(g1^7*y) + t^8.04/(g1^16*y) + (3*g1^10*t^8.1)/y + (6*g1*t^8.31)/y + (g1^18*t^8.58)/y + t^8.73/(g1^17*y) + (2*g1^9*t^8.79)/y - (t^4.38*y)/g1^2 - (2*t^6.45*y)/g1^5 - (t^6.66*y)/g1^14 + (t^7.14*y)/g1^6 + (2*t^7.35*y)/g1^15 + 2*g1^2*t^7.62*y + (3*t^7.83*y)/g1^7 + (t^8.04*y)/g1^16 + 3*g1^10*t^8.1*y + 6*g1*t^8.31*y + g1^18*t^8.58*y + (t^8.73*y)/g1^17 + 2*g1^9*t^8.79*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47181 | 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_2\phi_1^2$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1q_1q_2$ | 0.6791 | 0.8522 | 0.7969 | [X:[], M:[1.1508, 1.0793, 0.8492, 0.762, 0.6905], q:[0.381, 0.4682], qb:[0.5397, 0.7698], phi:[0.4603]] | t^2.07 + t^2.29 + t^2.55 + t^2.76 + t^3.02 + t^3.24 + t^3.45 + t^3.67 + t^3.93 + 2*t^4.14 + t^4.19 + t^4.36 + t^4.4 + t^4.57 + 2*t^4.62 + 2*t^4.83 + t^5.05 + 2*t^5.1 + 3*t^5.31 + 2*t^5.52 + t^5.57 + t^5.74 + t^5.79 + t^5.95 - t^4.38/y - t^4.38*y | detail |