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 |
|---|---|---|---|---|---|---|---|---|---|
| 202 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_1M_3$ + $ M_4q_1\tilde{q}_1$ | 0.7121 | 0.8517 | 0.8362 | [X:[], M:[0.8744, 1.1256, 1.1256, 0.8278], q:[0.5861, 0.5395], qb:[0.5861, 0.5395], phi:[0.4372]] | [X:[], M:[[0, -2, -2], [0, 2, 2], [0, 2, 2], [1, -4, -2]], q:[[-1, 2, 2], [1, 0, 0]], qb:[[0, 2, 0], [0, 0, 2]], phi:[[0, -1, -1]]] | 3 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ M_2$, $ M_3$, $ \tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_1q_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1^2$, $ M_4^2$, $ M_4q_2\tilde{q}_2$, $ M_2M_4$, $ M_3M_4$, $ M_4\tilde{q}_1\tilde{q}_2$ | . | -8 | t^2.48 + t^3.24 + 5*t^3.38 + 3*t^4.55 + 4*t^4.69 + 3*t^4.83 + t^4.97 + t^5.72 + t^5.86 - 8*t^6. - 4*t^6.14 + t^6.47 + 5*t^6.61 + 14*t^6.75 + 3*t^7.03 - 4*t^7.31 - 3*t^7.45 + 3*t^7.79 + 12*t^7.93 + 12*t^8.07 + 9*t^8.2 + t^8.34 - 5*t^8.48 + 3*t^8.76 + t^8.96 - t^4.31/y - t^6.8/y + t^7.83/y + t^8.72/y + (5*t^8.86)/y - t^4.31*y - t^6.8*y + t^7.83*y + t^8.72*y + 5*t^8.86*y | (g1*t^2.48)/(g2^4*g3^2) + g1*g3^2*t^3.24 + g1*g2^2*t^3.38 + 3*g2^2*g3^2*t^3.38 + (g2^2*g3^4*t^3.38)/g1 + (g1^2*t^4.55)/(g2*g3) + (g1*g3*t^4.55)/g2 + (g3^3*t^4.55)/g2 + (g1*g2*t^4.69)/g3 + 2*g2*g3*t^4.69 + (g2*g3^3*t^4.69)/g1 + (g2^3*t^4.83)/g3 + (g2^3*g3*t^4.83)/g1 + (g2^3*g3^3*t^4.83)/g1^2 + (g1^2*t^4.97)/(g2^8*g3^4) + (g1^2*t^5.72)/g2^4 + (g1*t^5.86)/g2^2 - 4*t^6. - (2*g1*t^6.)/g3^2 - (2*g3^2*t^6.)/g1 - (2*g2^2*t^6.14)/g1 - (g2^2*t^6.14)/g3^2 - (g2^2*g3^2*t^6.14)/g1^2 + g1^2*g3^4*t^6.47 + g1^2*g2^2*g3^2*t^6.61 + 3*g1*g2^2*g3^4*t^6.61 + g2^2*g3^6*t^6.61 + g1^2*g2^4*t^6.75 + 3*g1*g2^4*g3^2*t^6.75 + 6*g2^4*g3^4*t^6.75 + (3*g2^4*g3^6*t^6.75)/g1 + (g2^4*g3^8*t^6.75)/g1^2 + (g1^3*t^7.03)/(g2^5*g3^3) + (g1^2*t^7.03)/(g2^5*g3) + (g1*g3*t^7.03)/g2^5 - (g1*t^7.31)/(g2*g3^3) - (2*t^7.31)/(g2*g3) - (g3*t^7.31)/(g1*g2) + (g1^3*t^7.45)/(g2^12*g3^6) - (g2*t^7.45)/g3^3 - (2*g2*t^7.45)/(g1*g3) - (g2*g3*t^7.45)/g1^2 + (g1^3*g3*t^7.79)/g2 + (g1^2*g3^3*t^7.79)/g2 + (g1*g3^5*t^7.79)/g2 + (g1^3*g2*t^7.93)/g3 + 3*g1^2*g2*g3*t^7.93 + 4*g1*g2*g3^3*t^7.93 + 3*g2*g3^5*t^7.93 + (g2*g3^7*t^7.93)/g1 + (g1^2*g2^3*t^8.07)/g3 + 3*g1*g2^3*g3*t^8.07 + 4*g2^3*g3^3*t^8.07 + (3*g2^3*g3^5*t^8.07)/g1 + (g2^3*g3^7*t^8.07)/g1^2 + (g1^3*t^8.2)/(g2^8*g3^2) + (g1*g2^5*t^8.2)/g3 + 2*g2^5*g3*t^8.2 + (2*g2^5*g3^3*t^8.2)/g1 + (2*g2^5*g3^5*t^8.2)/g1^2 + (g2^5*g3^7*t^8.2)/g1^3 + (g1^2*t^8.34)/(g2^6*g3^2) - t^8.48/g2^4 - (g1^2*t^8.48)/(g2^4*g3^4) - (3*g1*t^8.48)/(g2^4*g3^2) + t^8.76/g1^2 + t^8.76/g3^4 + t^8.76/(g1*g3^2) + (g1^3*g3^2*t^8.96)/g2^4 - t^4.31/(g2*g3*y) - (g1*t^6.8)/(g2^5*g3^3*y) + (g2^3*g3*t^7.83)/(g1*y) + (g1^2*t^8.72)/(g2^4*y) + (3*g1*t^8.86)/(g2^2*y) + (g1^2*t^8.86)/(g2^2*g3^2*y) + (g3^2*t^8.86)/(g2^2*y) - (t^4.31*y)/(g2*g3) - (g1*t^6.8*y)/(g2^5*g3^3) + (g2^3*g3*t^7.83*y)/g1 + (g1^2*t^8.72*y)/g2^4 + (3*g1*t^8.86*y)/g2^2 + (g1^2*t^8.86*y)/(g2^2*g3^2) + (g3^2*t^8.86*y)/g2^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55769 | SU2adj1nf3 | $\phi_1q_1^2$ + $ M_1\phi_1^2$ + $ q_1q_2$ + $ M_2q_3\tilde{q}_1$ | 0.7121 | 0.8517 | 0.8362 | [X:[], M:[1.1256, 0.8278], q:[0.7814, 1.2186, 0.5861], qb:[0.5861, 0.5395, 0.5395], phi:[0.4372]] | t^2.48 + t^3.24 + 5*t^3.38 + 3*t^4.55 + 4*t^4.69 + 3*t^4.83 + t^4.97 + t^5.72 + t^5.86 - 8*t^6. - t^4.31/y - t^4.31*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 123 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_1M_3$ | 0.7003 | 0.8367 | 0.837 | [X:[], M:[0.9093, 1.0907, 1.0907], q:[0.5454, 0.5454], qb:[0.5454, 0.5454], phi:[0.4546]] | 7*t^3.27 + 10*t^4.64 - 16*t^6. - t^4.36/y - t^4.36*y | detail |