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 |
|---|---|---|---|---|---|---|---|---|---|
| 57022 | 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}_1\tilde{q}_2$ + $ M_1M_6$ + $ M_7\phi_1q_2^2$ + $ M_5^2$ | 0.6177 | 0.7934 | 0.7785 | [X:[], M:[1.2857, 0.9551, 0.7143, 0.7592, 1.0, 0.7143, 0.902], q:[0.3796, 0.3347], qb:[0.6653, 0.9061], phi:[0.4286]] | [X:[], M:[[0], [2], [0], [-2], [0], [0], [-2]], q:[[-1], [1]], qb:[[-1], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ M_6$, $ M_4$, $ \phi_1^2$, $ M_7$, $ M_2$, $ M_5$, $ \phi_1q_1q_2$, $ \phi_1q_1^2$, $ M_3^2$, $ M_3M_6$, $ M_6^2$, $ \phi_1q_2\tilde{q}_1$, $ M_3M_4$, $ M_4M_6$, $ \phi_1q_1\tilde{q}_1$, $ M_4^2$, $ M_3\phi_1^2$, $ M_6\phi_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_3M_7$, $ M_6M_7$, $ M_4\phi_1^2$, $ M_4M_7$, $ M_2M_3$, $ M_2M_6$, $ \phi_1q_2\tilde{q}_2$, $ M_2M_4$, $ M_3M_5$, $ M_5M_6$, $ \phi_1^4$, $ \phi_1q_1\tilde{q}_2$, $ M_4M_5$, $ M_7\phi_1^2$, $ \phi_1\tilde{q}_1^2$, $ M_7^2$, $ M_2\phi_1^2$, $ M_2M_7$, $ M_5\phi_1^2$, $ M_6\phi_1q_1q_2$, $ M_5M_7$, $ M_6\phi_1q_1^2$, $ M_4\phi_1q_1q_2$, $ M_2^2$, $ M_4\phi_1q_1^2$ | $\phi_1^3q_1q_2$ | -1 | 2*t^2.14 + t^2.28 + t^2.57 + t^2.71 + t^2.87 + t^3. + t^3.43 + t^3.56 + 3*t^4.29 + 2*t^4.42 + t^4.55 + 3*t^4.71 + 3*t^4.85 + t^4.98 + 2*t^5.01 + 4*t^5.14 + 2*t^5.28 + t^5.41 + t^5.44 + 3*t^5.57 + 3*t^5.71 + t^5.73 + t^5.84 - t^6. + t^6.13 + t^6.27 + 4*t^6.43 + 3*t^6.56 + 2*t^6.7 - t^6.72 + t^6.83 + 2*t^6.86 + 5*t^6.99 + 4*t^7.13 + t^7.15 + t^7.26 + 5*t^7.29 + 6*t^7.42 + 4*t^7.55 + 2*t^7.58 + t^7.69 + 6*t^7.71 + 6*t^7.85 + 2*t^7.87 + 4*t^7.98 + t^8.01 + 2*t^8.12 - 2*t^8.14 + t^8.28 + t^8.3 + 3*t^8.41 - t^8.44 + t^8.55 + 2*t^8.57 + t^8.6 + 2*t^8.71 + 4*t^8.84 - 5*t^8.87 + 3*t^8.98 - t^4.29/y - t^6.43/y - t^6.56/y - t^6.86/y - t^6.99/y - t^7.15/y + t^7.29/y + (3*t^7.42)/y + t^7.58/y + (3*t^7.71)/y + (3*t^7.85)/y + t^7.98/y + (3*t^8.01)/y + (4*t^8.14)/y + (2*t^8.28)/y + t^8.44/y + (3*t^8.57)/y + (3*t^8.71)/y + t^8.87/y - t^4.29*y - t^6.43*y - t^6.56*y - t^6.86*y - t^6.99*y - t^7.15*y + t^7.29*y + 3*t^7.42*y + t^7.58*y + 3*t^7.71*y + 3*t^7.85*y + t^7.98*y + 3*t^8.01*y + 4*t^8.14*y + 2*t^8.28*y + t^8.44*y + 3*t^8.57*y + 3*t^8.71*y + t^8.87*y | 2*t^2.14 + t^2.28/g1^2 + t^2.57 + t^2.71/g1^2 + g1^2*t^2.87 + t^3. + t^3.43 + t^3.56/g1^2 + 3*t^4.29 + (2*t^4.42)/g1^2 + t^4.55/g1^4 + 3*t^4.71 + (3*t^4.85)/g1^2 + t^4.98/g1^4 + 2*g1^2*t^5.01 + 4*t^5.14 + (2*t^5.28)/g1^2 + t^5.41/g1^4 + g1^2*t^5.44 + 3*t^5.57 + (3*t^5.71)/g1^2 + g1^4*t^5.73 + t^5.84/g1^4 - t^6. + t^6.13/g1^2 + t^6.27/g1^4 + 4*t^6.43 + (3*t^6.56)/g1^2 + (2*t^6.7)/g1^4 - g1^2*t^6.72 + t^6.83/g1^6 + 2*t^6.86 + (5*t^6.99)/g1^2 + (4*t^7.13)/g1^4 + g1^2*t^7.15 + t^7.26/g1^6 + 5*t^7.29 + (6*t^7.42)/g1^2 + (4*t^7.55)/g1^4 + 2*g1^2*t^7.58 + t^7.69/g1^6 + 6*t^7.71 + (6*t^7.85)/g1^2 + 2*g1^4*t^7.87 + (4*t^7.98)/g1^4 + g1^2*t^8.01 + (2*t^8.12)/g1^6 - 2*t^8.14 + t^8.28/g1^2 + g1^4*t^8.3 + (3*t^8.41)/g1^4 - g1^2*t^8.44 + t^8.55/g1^6 + 2*t^8.57 + g1^6*t^8.6 + (2*t^8.71)/g1^2 + (4*t^8.84)/g1^4 - 5*g1^2*t^8.87 + (3*t^8.98)/g1^6 - t^4.29/y - t^6.43/y - t^6.56/(g1^2*y) - t^6.86/y - t^6.99/(g1^2*y) - (g1^2*t^7.15)/y + t^7.29/y + (3*t^7.42)/(g1^2*y) + (g1^2*t^7.58)/y + (3*t^7.71)/y + (3*t^7.85)/(g1^2*y) + t^7.98/(g1^4*y) + (3*g1^2*t^8.01)/y + (4*t^8.14)/y + (2*t^8.28)/(g1^2*y) + (g1^2*t^8.44)/y + (3*t^8.57)/y + (3*t^8.71)/(g1^2*y) + (g1^2*t^8.87)/y - t^4.29*y - t^6.43*y - (t^6.56*y)/g1^2 - t^6.86*y - (t^6.99*y)/g1^2 - g1^2*t^7.15*y + t^7.29*y + (3*t^7.42*y)/g1^2 + g1^2*t^7.58*y + 3*t^7.71*y + (3*t^7.85*y)/g1^2 + (t^7.98*y)/g1^4 + 3*g1^2*t^8.01*y + 4*t^8.14*y + (2*t^8.28*y)/g1^2 + g1^2*t^8.44*y + 3*t^8.57*y + (3*t^8.71*y)/g1^2 + g1^2*t^8.87*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55473 | 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}_1\tilde{q}_2$ + $ M_1M_6$ + $ M_7\phi_1q_2^2$ | 0.6909 | 0.8877 | 0.7783 | [X:[], M:[1.1505, 0.7502, 0.8495, 0.7838, 0.6844, 0.8495, 0.7012], q:[0.3919, 0.4576], qb:[0.8579, 0.7586], phi:[0.3835]] | t^2.05 + t^2.1 + t^2.25 + t^2.3 + t^2.35 + 2*t^2.55 + t^3.5 + t^3.7 + t^4.11 + t^4.16 + t^4.21 + t^4.3 + 2*t^4.35 + 2*t^4.4 + t^4.46 + t^4.5 + t^4.55 + 4*t^4.6 + 3*t^4.65 + t^4.7 + 2*t^4.8 + 3*t^4.85 + 2*t^4.9 + 3*t^5.1 + t^5.56 + t^5.61 + t^5.75 + t^5.8 + t^5.85 - 2*t^6. - t^4.15/y - t^4.15*y | detail |