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 |
|---|---|---|---|---|---|---|---|---|---|
| 56068 | 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$ + $ M_2M_5$ + $ M_2M_6$ + $ \phi_1q_2^2$ + $ M_7\phi_1q_1^2$ | 0.6887 | 0.8828 | 0.7801 | [X:[], M:[0.8663, 1.1902, 1.1337, 0.7533, 0.8098, 0.8098, 0.7608], q:[0.3766, 0.7571], qb:[0.4331, 0.4896], phi:[0.4859]] | [X:[], M:[[14], [10], [-14], [-34], [-10], [-10], [40]], q:[[-17], [3]], qb:[[7], [31]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_7$, $ M_5$, $ M_6$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1^2$, $ M_3$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_4^2$, $ M_4M_7$, $ M_7^2$, $ M_4M_5$, $ M_4M_6$, $ M_5M_7$, $ M_6M_7$, $ M_1M_4$, $ M_5^2$, $ M_5M_6$, $ M_6^2$, $ \phi_1q_1q_2$, $ M_1M_7$, $ M_1M_5$, $ M_1M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_7\tilde{q}_1\tilde{q}_2$, $ M_4\phi_1^2$, $ M_1^2$, $ M_7\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_5\tilde{q}_1\tilde{q}_2$, $ M_6\tilde{q}_1\tilde{q}_2$, $ M_5\phi_1^2$, $ M_6\phi_1^2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ M_1\phi_1^2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_3M_7$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ M_3M_5$, $ M_3M_6$, $ \phi_1^4$ | . | -2 | t^2.26 + t^2.28 + 2*t^2.43 + t^2.6 + t^2.77 + t^2.92 + t^3.4 + t^3.89 + 2*t^4.06 + t^4.23 + t^4.4 + t^4.52 + t^4.54 + t^4.56 + 2*t^4.69 + 2*t^4.71 + 4*t^4.86 + t^4.88 + 3*t^5.03 + t^5.05 + t^5.18 + 4*t^5.2 + 2*t^5.34 + t^5.37 + t^5.51 + t^5.54 + 2*t^5.68 + t^5.83 - 2*t^6. + t^6.15 - t^6.17 + 4*t^6.32 + t^6.34 + 4*t^6.49 + t^6.51 + 4*t^6.66 + t^6.68 + t^6.78 + t^6.8 + 5*t^6.82 + t^6.85 + 2*t^6.95 + 2*t^6.97 + 4*t^6.99 + 3*t^7.12 + 2*t^7.14 + 2*t^7.16 + 5*t^7.29 + 3*t^7.31 + t^7.33 + t^7.44 + 5*t^7.46 + 3*t^7.48 + 2*t^7.6 + 5*t^7.63 + t^7.65 + 4*t^7.77 + 3*t^7.8 + t^7.82 + 3*t^7.94 + 4*t^7.97 - t^8.09 + 5*t^8.11 + t^8.14 - 2*t^8.26 + t^8.31 + t^8.41 - 7*t^8.43 + 2*t^8.45 + 3*t^8.58 - 4*t^8.6 + 2*t^8.62 + 6*t^8.75 - 3*t^8.77 + 2*t^8.79 + 5*t^8.92 + t^8.94 + t^8.96 - t^4.46/y - t^6.72/y - t^6.74/y - t^6.89/y - t^7.37/y + (2*t^7.54)/y + (2*t^7.69)/y + (2*t^7.71)/y + (2*t^7.86)/y + t^7.88/y + (4*t^8.03)/y + t^8.05/y + (2*t^8.18)/y + (4*t^8.2)/y + (2*t^8.34)/y + t^8.37/y + t^8.51/y + t^8.66/y + (2*t^8.68)/y + (2*t^8.83)/y - t^8.98/y - t^4.46*y - t^6.72*y - t^6.74*y - t^6.89*y - t^7.37*y + 2*t^7.54*y + 2*t^7.69*y + 2*t^7.71*y + 2*t^7.86*y + t^7.88*y + 4*t^8.03*y + t^8.05*y + 2*t^8.18*y + 4*t^8.2*y + 2*t^8.34*y + t^8.37*y + t^8.51*y + t^8.66*y + 2*t^8.68*y + 2*t^8.83*y - t^8.98*y | t^2.26/g1^34 + g1^40*t^2.28 + (2*t^2.43)/g1^10 + g1^14*t^2.6 + g1^38*t^2.77 + t^2.92/g1^12 + t^3.4/g1^14 + t^3.89/g1^16 + 2*g1^8*t^4.06 + g1^32*t^4.23 + g1^56*t^4.4 + t^4.52/g1^68 + g1^6*t^4.54 + g1^80*t^4.56 + (2*t^4.69)/g1^44 + 2*g1^30*t^4.71 + (4*t^4.86)/g1^20 + g1^54*t^4.88 + 3*g1^4*t^5.03 + g1^78*t^5.05 + t^5.18/g1^46 + 4*g1^28*t^5.2 + (2*t^5.34)/g1^22 + g1^52*t^5.37 + g1^2*t^5.51 + g1^76*t^5.54 + 2*g1^26*t^5.68 + t^5.83/g1^24 - 2*t^6. + t^6.15/g1^50 - g1^24*t^6.17 + (4*t^6.32)/g1^26 + g1^48*t^6.34 + (4*t^6.49)/g1^2 + g1^72*t^6.51 + 4*g1^22*t^6.66 + g1^96*t^6.68 + t^6.78/g1^102 + t^6.8/g1^28 + 5*g1^46*t^6.82 + g1^120*t^6.85 + (2*t^6.95)/g1^78 + (2*t^6.97)/g1^4 + 4*g1^70*t^6.99 + (3*t^7.12)/g1^54 + 2*g1^20*t^7.14 + 2*g1^94*t^7.16 + (5*t^7.29)/g1^30 + 3*g1^44*t^7.31 + g1^118*t^7.33 + t^7.44/g1^80 + (5*t^7.46)/g1^6 + 3*g1^68*t^7.48 + (2*t^7.6)/g1^56 + 5*g1^18*t^7.63 + g1^92*t^7.65 + (4*t^7.77)/g1^32 + 3*g1^42*t^7.8 + g1^116*t^7.82 + (3*t^7.94)/g1^8 + 4*g1^66*t^7.97 - t^8.09/g1^58 + 5*g1^16*t^8.11 + g1^90*t^8.14 - (2*t^8.26)/g1^34 + g1^114*t^8.31 + t^8.41/g1^84 - (7*t^8.43)/g1^10 + 2*g1^64*t^8.45 + (3*t^8.58)/g1^60 - 4*g1^14*t^8.6 + 2*g1^88*t^8.62 + (6*t^8.75)/g1^36 - 3*g1^38*t^8.77 + 2*g1^112*t^8.79 + (5*t^8.92)/g1^12 + g1^62*t^8.94 + g1^136*t^8.96 - t^4.46/(g1^6*y) - t^6.72/(g1^40*y) - (g1^34*t^6.74)/y - t^6.89/(g1^16*y) - t^7.37/(g1^18*y) + (2*g1^6*t^7.54)/y + (2*t^7.69)/(g1^44*y) + (2*g1^30*t^7.71)/y + (2*t^7.86)/(g1^20*y) + (g1^54*t^7.88)/y + (4*g1^4*t^8.03)/y + (g1^78*t^8.05)/y + (2*t^8.18)/(g1^46*y) + (4*g1^28*t^8.2)/y + (2*t^8.34)/(g1^22*y) + (g1^52*t^8.37)/y + (g1^2*t^8.51)/y + t^8.66/(g1^48*y) + (2*g1^26*t^8.68)/y + (2*t^8.83)/(g1^24*y) - t^8.98/(g1^74*y) - (t^4.46*y)/g1^6 - (t^6.72*y)/g1^40 - g1^34*t^6.74*y - (t^6.89*y)/g1^16 - (t^7.37*y)/g1^18 + 2*g1^6*t^7.54*y + (2*t^7.69*y)/g1^44 + 2*g1^30*t^7.71*y + (2*t^7.86*y)/g1^20 + g1^54*t^7.88*y + 4*g1^4*t^8.03*y + g1^78*t^8.05*y + (2*t^8.18*y)/g1^46 + 4*g1^28*t^8.2*y + (2*t^8.34*y)/g1^22 + g1^52*t^8.37*y + g1^2*t^8.51*y + (t^8.66*y)/g1^48 + 2*g1^26*t^8.68*y + (2*t^8.83*y)/g1^24 - (t^8.98*y)/g1^74 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 50910 | 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$ + $ M_2M_5$ + $ M_2M_6$ + $ \phi_1q_2^2$ | 0.6707 | 0.8503 | 0.7887 | [X:[], M:[0.8749, 1.1963, 1.1251, 0.7324, 0.8037, 0.8037], q:[0.3662, 0.7589], qb:[0.4374, 0.5087], phi:[0.4822]] | t^2.2 + 2*t^2.41 + t^2.62 + t^2.84 + t^2.89 + t^3.38 + t^3.64 + t^3.86 + 2*t^4.07 + t^4.28 + t^4.39 + t^4.5 + 2*t^4.61 + 4*t^4.82 + 3*t^5.04 + t^5.09 + 3*t^5.25 + 2*t^5.3 + t^5.46 + t^5.52 + t^5.68 + t^5.73 + t^5.79 + t^5.84 - 2*t^6. - t^4.45/y - t^4.45*y | detail |