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 |
|---|---|---|---|---|---|---|---|---|---|
| 4031 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2\tilde{q}_2$ + $ M_2M_5$ + $ M_4q_1q_2$ + $ M_6q_1\tilde{q}_2$ + $ M_7q_1q_2$ + $ M_4\phi_1\tilde{q}_2^2$ | 0.6795 | 0.867 | 0.7837 | [X:[], M:[0.8, 1.2, 0.8, 0.8, 0.8, 0.8, 0.8], q:[0.8, 0.4], qb:[0.8, 0.4], phi:[0.4]] | [X:[], M:[[0], [0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 1359/2000, c: 867/1000, M1: 4/5, M2: 6/5, M3: 4/5, M4: 4/5, M5: 4/5, M6: 4/5, M7: 4/5, q1: 4/5, q2: 2/5, qb1: 4/5, qb2: 2/5, phi1: 2/5} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ M_3$, $ M_4$, $ M_5$, $ M_6$, $ M_7$, $ \phi_1^2$, $ \phi_1q_2^2$, $ \phi_1\tilde{q}_2^2$, $ M_1^2$, $ M_1M_3$, $ M_3^2$, $ M_1M_4$, $ M_3M_4$, $ M_4^2$, $ M_1M_5$, $ M_3M_5$, $ M_4M_5$, $ M_5^2$, $ M_1M_6$, $ M_3M_6$, $ M_4M_6$, $ M_5M_6$, $ M_6^2$, $ M_1M_7$, $ M_3M_7$, $ M_4M_7$, $ M_5M_7$, $ M_6M_7$, $ M_7^2$, $ M_1\phi_1^2$, $ M_3\phi_1^2$, $ M_4\phi_1^2$, $ M_5\phi_1^2$, $ M_6\phi_1^2$, $ M_7\phi_1^2$, $ \phi_1^4$, $ q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$ | $M_3\phi_1q_2^2$, $ M_4\phi_1q_2^2$, $ M_5\phi_1q_2^2$, $ M_6\phi_1q_2^2$, $ M_7\phi_1q_2^2$, $ \phi_1^3q_2^2$, $ \phi_1\tilde{q}_1^2$, $ M_1\phi_1\tilde{q}_2^2$, $ M_3\phi_1\tilde{q}_2^2$, $ M_5\phi_1\tilde{q}_2^2$, $ M_6\phi_1\tilde{q}_2^2$, $ M_7\phi_1\tilde{q}_2^2$, $ \phi_1^3\tilde{q}_2^2$ | 5 | 7*t^2.4 + 2*t^3.6 + 29*t^4.8 + 5*t^6. + 77*t^7.2 - 12*t^8.4 - t^4.2/y - (6*t^6.6)/y + (27*t^7.8)/y - t^4.2*y - 6*t^6.6*y + 27*t^7.8*y | 7*t^2.4 + 2*t^3.6 + 29*t^4.8 + 5*t^6. + 77*t^7.2 - 12*t^8.4 - t^4.2/y - (6*t^6.6)/y + (27*t^7.8)/y - t^4.2*y - 6*t^6.6*y + 27*t^7.8*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1639 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2\tilde{q}_2$ + $ M_2M_5$ + $ M_4q_1q_2$ + $ M_6q_1\tilde{q}_2$ + $ M_7q_1q_2$ | 0.7025 | 0.89 | 0.7893 | [X:[], M:[0.849, 1.151, 0.9714, 0.7265, 0.849, 0.849, 0.7265], q:[0.7878, 0.4857], qb:[0.6653, 0.3633], phi:[0.4245]] | 2*t^2.18 + 4*t^2.55 + t^2.91 + t^3.45 + t^4.19 + 5*t^4.36 + 9*t^4.73 + 11*t^5.09 + t^5.27 + 3*t^5.46 + t^5.63 + t^5.83 - t^4.27/y - t^4.27*y | detail |