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 |
|---|---|---|---|---|---|---|---|---|---|
| 56247 | 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_1^2$ + $ M_6\phi_1q_1^2$ + $ M_2M_6$ + $ M_7\tilde{q}_1\tilde{q}_2$ | 0.6719 | 0.8474 | 0.7929 | [X:[], M:[1.1154, 1.1541, 0.8846, 0.6924, 1.0767, 0.8459, 0.7311], q:[0.3462, 0.5384], qb:[0.4997, 0.7692], phi:[0.4616]] | [X:[], M:[[-1], [-10], [1], [-6], [8], [10], [-15]], q:[[-3], [4]], qb:[[13], [2]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_7$, $ M_6$, $ M_3$, $ q_2\tilde{q}_1$, $ M_5$, $ M_1$, $ M_2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1q_2$, $ M_4^2$, $ M_4M_7$, $ \phi_1\tilde{q}_1^2$, $ M_7^2$, $ \phi_1q_2\tilde{q}_1$, $ M_4M_6$, $ \phi_1q_2^2$, $ M_3M_4$, $ M_6M_7$, $ \phi_1q_1\tilde{q}_2$, $ M_3M_7$, $ M_6^2$, $ M_3M_6$, $ M_4q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ M_4M_5$, $ M_7q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ M_1M_4$, $ M_5M_7$, $ M_2M_4$, $ M_1M_7$, $ M_6q_2\tilde{q}_1$, $ M_2M_7$, $ M_5M_6$, $ M_3q_2\tilde{q}_1$, $ M_3M_5$, $ M_1M_6$ | $M_4\phi_1q_1\tilde{q}_1$ | 0 | t^2.08 + t^2.19 + t^2.54 + t^2.65 + t^3.11 + t^3.23 + t^3.35 + t^3.46 + t^3.92 + t^4.04 + t^4.15 + t^4.27 + t^4.38 + t^4.39 + t^4.5 + 2*t^4.62 + 2*t^4.73 + t^4.85 + t^5.08 + 2*t^5.19 + 3*t^5.31 + t^5.42 + t^5.54 + t^5.65 + t^5.66 + 2*t^5.77 + t^5.88 + t^6.12 + 3*t^6.23 + t^6.34 + t^6.35 + 3*t^6.46 + 4*t^6.58 + 3*t^6.69 + 2*t^6.81 + 3*t^6.92 + 3*t^7.04 + 3*t^7.15 + 2*t^7.27 + 3*t^7.38 + 4*t^7.5 + 2*t^7.61 + t^7.62 + 4*t^7.73 + 4*t^7.85 + 2*t^7.96 + 5*t^8.31 + 3*t^8.42 + 2*t^8.43 + 2*t^8.54 + t^8.66 + 6*t^8.77 + 3*t^8.88 + 2*t^8.89 - t^4.38/y - t^6.46/y - t^6.58/y + t^7.27/y + t^7.62/y + (2*t^7.73)/y + t^7.85/y + (3*t^8.19)/y + (3*t^8.31)/y + (2*t^8.42)/y + t^8.54/y + t^8.65/y + t^8.77/y + (2*t^8.88)/y - t^4.38*y - t^6.46*y - t^6.58*y + t^7.27*y + t^7.62*y + 2*t^7.73*y + t^7.85*y + 3*t^8.19*y + 3*t^8.31*y + 2*t^8.42*y + t^8.54*y + t^8.65*y + t^8.77*y + 2*t^8.88*y | t^2.08/g1^6 + t^2.19/g1^15 + g1^10*t^2.54 + g1*t^2.65 + g1^17*t^3.11 + g1^8*t^3.23 + t^3.35/g1 + t^3.46/g1^10 + g1^6*t^3.92 + t^4.04/g1^3 + t^4.15/g1^12 + t^4.27/g1^21 + g1^22*t^4.38 + t^4.39/g1^30 + g1^13*t^4.5 + 2*g1^4*t^4.62 + (2*t^4.73)/g1^5 + t^4.85/g1^14 + g1^20*t^5.08 + 2*g1^11*t^5.19 + 3*g1^2*t^5.31 + t^5.42/g1^7 + t^5.54/g1^16 + g1^27*t^5.65 + t^5.66/g1^25 + 2*g1^18*t^5.77 + g1^9*t^5.88 + t^6.12/g1^9 + (2*t^6.23)/g1^18 + g1^34*t^6.23 + g1^25*t^6.34 + t^6.35/g1^27 + t^6.46/g1^36 + 2*g1^16*t^6.46 + t^6.58/g1^45 + 3*g1^7*t^6.58 + (3*t^6.69)/g1^2 + (2*t^6.81)/g1^11 + (2*t^6.92)/g1^20 + g1^32*t^6.92 + t^7.04/g1^29 + 2*g1^23*t^7.04 + 3*g1^14*t^7.15 + 2*g1^5*t^7.27 + (3*t^7.38)/g1^4 + (3*t^7.5)/g1^13 + g1^39*t^7.5 + 2*g1^30*t^7.61 + t^7.62/g1^22 + t^7.73/g1^31 + 3*g1^21*t^7.73 + t^7.85/g1^40 + 3*g1^12*t^7.85 + 2*g1^3*t^7.96 - t^8.19/g1^15 + g1^37*t^8.19 + (2*t^8.31)/g1^24 + 3*g1^28*t^8.31 + 3*g1^19*t^8.42 + (2*t^8.43)/g1^33 + t^8.54/g1^42 + g1^10*t^8.54 + t^8.66/g1^51 + t^8.77/g1^60 + (3*t^8.77)/g1^8 + 2*g1^44*t^8.77 + 3*g1^35*t^8.88 + (2*t^8.89)/g1^17 - t^4.38/(g1^4*y) - t^6.46/(g1^10*y) - t^6.58/(g1^19*y) + t^7.27/(g1^21*y) + (g1^4*t^7.62)/y + (2*t^7.73)/(g1^5*y) + t^7.85/(g1^14*y) + (3*g1^11*t^8.19)/y + (3*g1^2*t^8.31)/y + (2*t^8.42)/(g1^7*y) + t^8.54/(g1^16*y) + (g1^27*t^8.65)/y - t^8.77/(g1^34*y) + (2*g1^18*t^8.77)/y + (2*g1^9*t^8.88)/y - (t^4.38*y)/g1^4 - (t^6.46*y)/g1^10 - (t^6.58*y)/g1^19 + (t^7.27*y)/g1^21 + g1^4*t^7.62*y + (2*t^7.73*y)/g1^5 + (t^7.85*y)/g1^14 + 3*g1^11*t^8.19*y + 3*g1^2*t^8.31*y + (2*t^8.42*y)/g1^7 + (t^8.54*y)/g1^16 + g1^27*t^8.65*y - (t^8.77*y)/g1^34 + 2*g1^18*t^8.77*y + 2*g1^9*t^8.88*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 |
|---|---|---|---|---|---|---|---|---|---|
| 51554 | 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_1^2$ + $ M_6\phi_1q_1^2$ + $ M_2M_6$ | 0.6525 | 0.8129 | 0.8027 | [X:[], M:[1.1167, 1.1666, 0.8833, 0.7, 1.0667, 0.8334], q:[0.35, 0.5334], qb:[0.4834, 0.7667], phi:[0.4666]] | t^2.1 + t^2.5 + t^2.65 + t^3.05 + t^3.2 + t^3.35 + t^3.5 + t^3.75 + t^3.9 + t^4.05 + t^4.2 + t^4.3 + t^4.45 + 2*t^4.6 + t^4.75 + t^5. + 2*t^5.15 + 2*t^5.3 + t^5.55 + 2*t^5.7 + 2*t^5.85 - t^4.4/y - t^4.4*y | detail |