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 |
|---|---|---|---|---|---|---|---|---|---|
| 55543 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1^4$ + $ \phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_4\phi_1q_2^2$ + $ M_4q_1\tilde{q}_2$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_1\tilde{q}_2$ | 0.666 | 0.8608 | 0.7736 | [X:[], M:[1.1459, 1.118, 0.7083, 0.7639, 0.882, 0.7639], q:[0.4861, 0.368], qb:[0.3959, 0.75], phi:[0.5]] | [X:[], M:[[3], [-1], [-6], [2], [1], [2]], q:[[-2], [-1]], qb:[[3], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ M_4$, $ M_6$, $ q_2\tilde{q}_1$, $ M_5$, $ \phi_1^2$, $ M_2$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_1q_2$, $ \phi_1q_1\tilde{q}_1$, $ M_3^2$, $ M_3M_4$, $ M_3M_6$, $ \phi_1q_1^2$, $ M_3q_2\tilde{q}_1$, $ M_4^2$, $ M_4M_6$, $ M_6^2$, $ M_4q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_3M_5$, $ M_4M_5$, $ M_5M_6$, $ M_5q_2\tilde{q}_1$, $ M_3\phi_1^2$, $ M_5^2$, $ M_4\phi_1^2$, $ M_6\phi_1^2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_2M_3$, $ M_1M_3$, $ M_3\tilde{q}_1\tilde{q}_2$, $ M_2M_4$, $ M_2M_6$, $ M_5\phi_1^2$, $ M_2q_2\tilde{q}_1$, $ M_1M_4$, $ M_1M_6$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_6\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$ | $M_2M_5$ | -2 | t^2.12 + 3*t^2.29 + t^2.65 + t^3. + t^3.35 + 2*t^3.44 + t^3.79 + t^4.06 + t^4.15 + t^4.25 + 4*t^4.42 + 6*t^4.58 + t^4.77 + 3*t^4.94 + t^5.12 + 4*t^5.29 + t^5.48 + 2*t^5.56 + 3*t^5.65 + 5*t^5.73 - 2*t^6. + 4*t^6.08 + t^6.19 + t^6.35 + t^6.37 + 4*t^6.44 + 4*t^6.54 + 8*t^6.71 + 2*t^6.79 + 12*t^6.88 + t^6.9 + 3*t^7.06 - 2*t^7.15 + 6*t^7.23 + t^7.25 + 3*t^7.42 - t^7.5 + 9*t^7.58 + t^7.6 + 2*t^7.69 + 2*t^7.77 + 4*t^7.85 + 6*t^7.94 + 9*t^8.02 - 2*t^8.12 + t^8.21 - 6*t^8.29 + t^8.31 + 8*t^8.38 + 2*t^8.48 + t^8.5 + t^8.56 - 3*t^8.65 + 4*t^8.67 + 9*t^8.73 + 9*t^8.83 - t^4.5/y - t^6.62/y - (2*t^6.79)/y + t^7.06/y + (3*t^7.42)/y + (3*t^7.58)/y + t^7.77/y + (2*t^7.94)/y + t^8.12/y + (2*t^8.21)/y + (3*t^8.29)/y + t^8.38/y + t^8.48/y + (2*t^8.56)/y + (4*t^8.65)/y + (6*t^8.73)/y - t^8.75/y - t^8.92/y - t^4.5*y - t^6.62*y - 2*t^6.79*y + t^7.06*y + 3*t^7.42*y + 3*t^7.58*y + t^7.77*y + 2*t^7.94*y + t^8.12*y + 2*t^8.21*y + 3*t^8.29*y + t^8.38*y + t^8.48*y + 2*t^8.56*y + 4*t^8.65*y + 6*t^8.73*y - t^8.75*y - t^8.92*y | t^2.12/g1^6 + 3*g1^2*t^2.29 + g1*t^2.65 + t^3. + t^3.35/g1 + 2*g1^3*t^3.44 + g1^2*t^3.79 + t^4.06/g1^3 + g1*t^4.15 + t^4.25/g1^12 + (4*t^4.42)/g1^4 + 6*g1^4*t^4.58 + t^4.77/g1^5 + 3*g1^3*t^4.94 + t^5.12/g1^6 + 4*g1^2*t^5.29 + t^5.48/g1^7 + (2*t^5.56)/g1^3 + 3*g1*t^5.65 + 5*g1^5*t^5.73 - 2*t^6. + 4*g1^4*t^6.08 + t^6.19/g1^9 + t^6.35/g1 + t^6.37/g1^18 + 4*g1^3*t^6.44 + (4*t^6.54)/g1^10 + (8*t^6.71)/g1^2 + 2*g1^2*t^6.79 + 12*g1^6*t^6.88 + t^6.9/g1^11 + (3*t^7.06)/g1^3 - 2*g1*t^7.15 + 6*g1^5*t^7.23 + t^7.25/g1^12 + (3*t^7.42)/g1^4 - t^7.5 + 9*g1^4*t^7.58 + t^7.6/g1^13 + (2*t^7.69)/g1^9 + (2*t^7.77)/g1^5 + (4*t^7.85)/g1 + 6*g1^3*t^7.94 + 9*g1^7*t^8.02 - (2*t^8.12)/g1^6 + t^8.21/g1^2 - 6*g1^2*t^8.29 + t^8.31/g1^15 + 8*g1^6*t^8.38 + (2*t^8.48)/g1^7 + t^8.5/g1^24 + t^8.56/g1^3 - 3*g1*t^8.65 + (4*t^8.67)/g1^16 + 9*g1^5*t^8.73 + (9*t^8.83)/g1^8 - t^4.5/y - t^6.62/(g1^6*y) - (2*g1^2*t^6.79)/y + t^7.06/(g1^3*y) + (3*t^7.42)/(g1^4*y) + (3*g1^4*t^7.58)/y + t^7.77/(g1^5*y) + (2*g1^3*t^7.94)/y + t^8.12/(g1^6*y) + (2*t^8.21)/(g1^2*y) + (3*g1^2*t^8.29)/y + (g1^6*t^8.38)/y + t^8.48/(g1^7*y) + (2*t^8.56)/(g1^3*y) + (4*g1*t^8.65)/y + (6*g1^5*t^8.73)/y - t^8.75/(g1^12*y) - t^8.92/(g1^4*y) - t^4.5*y - (t^6.62*y)/g1^6 - 2*g1^2*t^6.79*y + (t^7.06*y)/g1^3 + (3*t^7.42*y)/g1^4 + 3*g1^4*t^7.58*y + (t^7.77*y)/g1^5 + 2*g1^3*t^7.94*y + (t^8.12*y)/g1^6 + (2*t^8.21*y)/g1^2 + 3*g1^2*t^8.29*y + g1^6*t^8.38*y + (t^8.48*y)/g1^7 + (2*t^8.56*y)/g1^3 + 4*g1*t^8.65*y + 6*g1^5*t^8.73*y - (t^8.75*y)/g1^12 - (t^8.92*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 47085 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1^4$ + $ \phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_4\phi_1q_2^2$ + $ M_4q_1\tilde{q}_2$ + $ M_5q_2\tilde{q}_2$ | 0.6476 | 0.8279 | 0.7823 | [X:[], M:[1.1521, 1.116, 0.6958, 0.7681, 0.884], q:[0.4819, 0.366], qb:[0.4021, 0.75], phi:[0.5]] | t^2.09 + 2*t^2.3 + t^2.65 + t^3. + t^3.35 + 2*t^3.46 + t^3.7 + t^3.8 + t^4.04 + t^4.15 + t^4.17 + 3*t^4.39 + 3*t^4.61 + t^4.74 + 2*t^4.96 + t^5.09 + 3*t^5.3 + t^5.44 + 2*t^5.54 + 2*t^5.65 + 3*t^5.76 + t^5.78 - t^4.5/y - t^4.5*y | detail |