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 |
|---|---|---|---|---|---|---|---|---|---|
| 56438 | 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_4\phi_1q_1^2$ + $ M_5\phi_1q_1^2$ + $ M_6\phi_1q_1q_2$ + $ M_7\phi_1^2$ | 0.6907 | 0.8714 | 0.7926 | [X:[], M:[1.1584, 1.0497, 0.8416, 0.7723, 0.7723, 0.7029, 1.089], q:[0.3861, 0.4555], qb:[0.5642, 0.7723], phi:[0.4555]] | [X:[], M:[[3], [-18], [-3], [2], [2], [7], [8]], 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_5$, $ M_3$, $ q_2\tilde{q}_1$, $ M_2$, $ M_7$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4M_6$, $ M_5M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_4^2$, $ M_4M_5$, $ M_5^2$, $ M_3M_6$, $ \phi_1\tilde{q}_1^2$, $ M_3M_4$, $ M_3M_5$, $ \phi_1q_1\tilde{q}_2$, $ M_3^2$, $ \phi_1q_2\tilde{q}_2$, $ M_6q_2\tilde{q}_1$, $ M_2M_6$, $ M_6M_7$, $ M_4q_2\tilde{q}_1$, $ M_5q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2M_4$, $ M_2M_5$, $ M_1M_6$, $ M_4M_7$, $ M_5M_7$, $ M_3q_2\tilde{q}_1$, $ M_1M_4$, $ M_1M_5$, $ M_3M_7$ | . | -2 | t^2.11 + 2*t^2.32 + t^2.52 + t^3.06 + t^3.15 + t^3.27 + t^3.48 + t^4.01 + t^4.1 + 2*t^4.22 + 3*t^4.43 + 4*t^4.63 + t^4.75 + 2*t^4.84 + t^5.05 + t^5.17 + t^5.26 + 3*t^5.38 + t^5.47 + 4*t^5.58 + 2*t^5.79 - 2*t^6. + 2*t^6.12 + t^6.3 + 4*t^6.33 + 2*t^6.42 + 6*t^6.53 + t^6.62 + 6*t^6.74 - t^6.83 + t^6.86 + 5*t^6.95 - t^7.04 + 3*t^7.07 + 3*t^7.16 + t^7.25 + 3*t^7.28 + t^7.37 + 5*t^7.48 + 2*t^7.57 + 6*t^7.69 + t^7.81 + 6*t^7.9 - t^7.99 + t^8.02 + t^8.2 + 3*t^8.23 - 5*t^8.32 + t^8.41 + 6*t^8.43 - 2*t^8.52 + 2*t^8.61 + 9*t^8.64 + t^8.73 + t^8.76 + 11*t^8.85 - t^8.94 + 2*t^8.97 - t^4.37/y - t^6.48/y - (2*t^6.68)/y + t^7.22/y + (2*t^7.43)/y - t^7.52/y + (2*t^7.63)/y + (2*t^7.84)/y + (2*t^8.05)/y + t^8.17/y + (2*t^8.26)/y + (3*t^8.38)/y + (2*t^8.47)/y + (3*t^8.58)/y + t^8.67/y + t^8.79/y - t^4.37*y - t^6.48*y - 2*t^6.68*y + t^7.22*y + 2*t^7.43*y - t^7.52*y + 2*t^7.63*y + 2*t^7.84*y + 2*t^8.05*y + t^8.17*y + 2*t^8.26*y + 3*t^8.38*y + 2*t^8.47*y + 3*t^8.58*y + t^8.67*y + t^8.79*y | g1^7*t^2.11 + 2*g1^2*t^2.32 + t^2.52/g1^3 + g1^13*t^3.06 + t^3.15/g1^18 + g1^8*t^3.27 + g1^3*t^3.48 + g1^19*t^4.01 + t^4.1/g1^12 + 2*g1^14*t^4.22 + 3*g1^9*t^4.43 + 4*g1^4*t^4.63 + g1^30*t^4.75 + (2*t^4.84)/g1 + t^5.05/g1^6 + g1^20*t^5.17 + t^5.26/g1^11 + 3*g1^15*t^5.38 + t^5.47/g1^16 + 4*g1^10*t^5.58 + 2*g1^5*t^5.79 - 2*t^6. + 2*g1^26*t^6.12 + t^6.3/g1^36 + 4*g1^21*t^6.33 + (2*t^6.42)/g1^10 + 6*g1^16*t^6.53 + t^6.62/g1^15 + 6*g1^11*t^6.74 - t^6.83/g1^20 + g1^37*t^6.86 + 5*g1^6*t^6.95 - t^7.04/g1^25 + 3*g1^32*t^7.07 + 3*g1*t^7.16 + t^7.25/g1^30 + 3*g1^27*t^7.28 + t^7.37/g1^4 + 5*g1^22*t^7.48 + (2*t^7.57)/g1^9 + 6*g1^17*t^7.69 + g1^43*t^7.81 + 6*g1^12*t^7.9 - t^7.99/g1^19 + g1^38*t^8.02 + t^8.2/g1^24 + 3*g1^33*t^8.23 - 5*g1^2*t^8.32 + t^8.41/g1^29 + 6*g1^28*t^8.43 - (2*t^8.52)/g1^3 + (2*t^8.61)/g1^34 + 9*g1^23*t^8.64 + t^8.73/g1^8 + g1^49*t^8.76 + 11*g1^18*t^8.85 - t^8.94/g1^13 + 2*g1^44*t^8.97 - t^4.37/(g1^4*y) - (g1^3*t^6.48)/y - (2*t^6.68)/(g1^2*y) + (g1^14*t^7.22)/y + (2*g1^9*t^7.43)/y - t^7.52/(g1^22*y) + (2*g1^4*t^7.63)/y + (2*t^7.84)/(g1*y) + (2*t^8.05)/(g1^6*y) + (g1^20*t^8.17)/y + (2*t^8.26)/(g1^11*y) + (3*g1^15*t^8.38)/y + (2*t^8.47)/(g1^16*y) + (3*g1^10*t^8.58)/y + t^8.67/(g1^21*y) + (g1^5*t^8.79)/y - (t^4.37*y)/g1^4 - g1^3*t^6.48*y - (2*t^6.68*y)/g1^2 + g1^14*t^7.22*y + 2*g1^9*t^7.43*y - (t^7.52*y)/g1^22 + 2*g1^4*t^7.63*y + (2*t^7.84*y)/g1 + (2*t^8.05*y)/g1^6 + g1^20*t^8.17*y + (2*t^8.26*y)/g1^11 + 3*g1^15*t^8.38*y + (2*t^8.47*y)/g1^16 + 3*g1^10*t^8.58*y + (t^8.67*y)/g1^21 + g1^5*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 |
|---|---|---|---|---|---|---|---|---|---|
| 53383 | 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_4\phi_1q_1^2$ + $ M_5\phi_1q_1^2$ + $ M_6\phi_1q_1q_2$ | 0.6993 | 0.8844 | 0.7907 | [X:[], M:[1.1626, 1.0246, 0.8374, 0.775, 0.775, 0.7127], q:[0.3875, 0.4499], qb:[0.5879, 0.775], phi:[0.4499]] | t^2.14 + 2*t^2.33 + t^2.51 + t^2.7 + t^3.07 + t^3.11 + t^3.49 + t^4.05 + t^4.09 + 2*t^4.28 + 3*t^4.46 + 4*t^4.65 + 3*t^4.84 + t^4.88 + 3*t^5.02 + 2*t^5.21 + t^5.25 + 2*t^5.4 + 2*t^5.44 + 2*t^5.63 + t^5.77 + 2*t^5.81 - 2*t^6. - t^4.35/y - t^4.35*y | detail |