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 |
|---|---|---|---|---|---|---|---|---|---|
| 56205 | 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_7\phi_1q_1^2$ | 0.7043 | 0.8918 | 0.7897 | [X:[], M:[1.1698, 0.9814, 0.8302, 0.7798, 0.931, 0.7294, 0.7798], q:[0.3899, 0.4403], qb:[0.6287, 0.7798], phi:[0.4403]] | [X:[], M:[[3], [-18], [-3], [2], [-13], [7], [2]], 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_7$, $ M_3$, $ \phi_1^2$, $ M_5$, $ M_2$, $ M_1$, $ \phi_1q_2^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4M_6$, $ M_6M_7$, $ \phi_1q_2\tilde{q}_1$, $ M_4^2$, $ M_3M_6$, $ M_4M_7$, $ M_7^2$, $ M_3M_4$, $ M_3M_7$, $ M_6\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_3^2$, $ M_5M_6$, $ M_4\phi_1^2$, $ M_7\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ M_4M_5$, $ M_2M_6$, $ M_5M_7$, $ M_3\phi_1^2$, $ M_2M_4$, $ M_3M_5$, $ M_2M_7$, $ \phi_1^4$, $ M_2M_3$, $ M_5\phi_1^2$, $ M_5^2$, $ M_2\phi_1^2$, $ M_1M_6$, $ M_2M_5$, $ M_1M_4$, $ M_1M_7$, $ M_2^2$ | . | -2 | t^2.19 + 2*t^2.34 + t^2.49 + t^2.64 + t^2.79 + t^2.94 + t^3.51 + t^3.96 + t^4.23 + 2*t^4.38 + 3*t^4.53 + 4*t^4.68 + 3*t^4.83 + 4*t^4.98 + t^5.09 + 4*t^5.13 + 3*t^5.28 + t^5.43 + 2*t^5.59 + t^5.7 + t^5.74 + t^5.85 + t^5.89 - 2*t^6. + 2*t^6.3 + t^6.41 + t^6.45 + 3*t^6.57 + 4*t^6.72 + 6*t^6.87 + t^6.91 + 8*t^7.02 + 7*t^7.17 + t^7.28 + 7*t^7.32 + 2*t^7.43 + 9*t^7.47 + 6*t^7.62 + t^7.73 + 5*t^7.77 + 7*t^7.93 + 4*t^8.08 - 3*t^8.19 + 4*t^8.23 - 6*t^8.34 + 2*t^8.38 - 2*t^8.49 + 2*t^8.53 + 2*t^8.6 - t^8.64 + t^8.68 + 3*t^8.75 - 3*t^8.79 + t^8.83 + 4*t^8.9 - 3*t^8.94 - t^4.32/y - t^6.51/y - (2*t^6.66)/y - t^6.96/y - t^7.11/y - t^7.27/y + t^7.38/y + (3*t^7.53)/y + (3*t^7.68)/y + (3*t^7.83)/y + (5*t^7.98)/y + (5*t^8.13)/y + (3*t^8.28)/y + (2*t^8.43)/y + t^8.59/y + t^8.74/y - t^4.32*y - t^6.51*y - 2*t^6.66*y - t^6.96*y - t^7.11*y - t^7.27*y + t^7.38*y + 3*t^7.53*y + 3*t^7.68*y + 3*t^7.83*y + 5*t^7.98*y + 5*t^8.13*y + 3*t^8.28*y + 2*t^8.43*y + t^8.59*y + t^8.74*y | g1^7*t^2.19 + 2*g1^2*t^2.34 + t^2.49/g1^3 + t^2.64/g1^8 + t^2.79/g1^13 + t^2.94/g1^18 + g1^3*t^3.51 + t^3.96/g1^12 + g1^19*t^4.23 + 2*g1^14*t^4.38 + 3*g1^9*t^4.53 + 4*g1^4*t^4.68 + (3*t^4.83)/g1 + (4*t^4.98)/g1^6 + g1^30*t^5.09 + (4*t^5.13)/g1^11 + (3*t^5.28)/g1^16 + t^5.43/g1^21 + (2*t^5.59)/g1^26 + g1^10*t^5.7 + t^5.74/g1^31 + g1^5*t^5.85 + t^5.89/g1^36 - 2*t^6. + (2*t^6.3)/g1^10 + g1^26*t^6.41 + t^6.45/g1^15 + 3*g1^21*t^6.57 + 4*g1^16*t^6.72 + 6*g1^11*t^6.87 + t^6.91/g1^30 + 8*g1^6*t^7.02 + 7*g1*t^7.17 + g1^37*t^7.28 + (7*t^7.32)/g1^4 + 2*g1^32*t^7.43 + (9*t^7.47)/g1^9 + (6*t^7.62)/g1^14 + g1^22*t^7.73 + (5*t^7.77)/g1^19 + (7*t^7.93)/g1^24 + (4*t^8.08)/g1^29 - 3*g1^7*t^8.19 + (4*t^8.23)/g1^34 - 6*g1^2*t^8.34 + (2*t^8.38)/g1^39 - (2*t^8.49)/g1^3 + (2*t^8.53)/g1^44 + 2*g1^33*t^8.6 - t^8.64/g1^8 + t^8.68/g1^49 + 3*g1^28*t^8.75 - (3*t^8.79)/g1^13 + t^8.83/g1^54 + 4*g1^23*t^8.9 - (3*t^8.94)/g1^18 - t^4.32/(g1^4*y) - (g1^3*t^6.51)/y - (2*t^6.66)/(g1^2*y) - t^6.96/(g1^12*y) - t^7.11/(g1^17*y) - t^7.27/(g1^22*y) + (g1^14*t^7.38)/y + (3*g1^9*t^7.53)/y + (3*g1^4*t^7.68)/y + (3*t^7.83)/(g1*y) + (5*t^7.98)/(g1^6*y) + (5*t^8.13)/(g1^11*y) + (3*t^8.28)/(g1^16*y) + (2*t^8.43)/(g1^21*y) + t^8.59/(g1^26*y) + t^8.74/(g1^31*y) - (t^4.32*y)/g1^4 - g1^3*t^6.51*y - (2*t^6.66*y)/g1^2 - (t^6.96*y)/g1^12 - (t^7.11*y)/g1^17 - (t^7.27*y)/g1^22 + g1^14*t^7.38*y + 3*g1^9*t^7.53*y + 3*g1^4*t^7.68*y + (3*t^7.83*y)/g1 + (5*t^7.98*y)/g1^6 + (5*t^8.13*y)/g1^11 + (3*t^8.28*y)/g1^16 + (2*t^8.43*y)/g1^21 + (t^8.59*y)/g1^26 + (t^8.74*y)/g1^31 |
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 |