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 |
|---|---|---|---|---|---|---|---|---|---|
| 46336 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_2\tilde{q}_1$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4\phi_1q_1\tilde{q}_2$ | 0.6895 | 0.8749 | 0.7881 | [X:[], M:[0.6958, 0.6865, 0.6958, 0.6958], q:[0.4828, 0.8214], qb:[0.8307, 0.4736], phi:[0.3479]] | [X:[], M:[[-2, -2], [-5, -1], [-2, -2], [-2, -2]], q:[[3, 1], [-1, 1]], qb:[[2, 0], [0, 2]], phi:[[-1, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ M_1$, $ M_3$, $ M_4$, $ \phi_1^2$, $ q_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_1^2$, $ M_2^2$, $ M_1M_2$, $ M_2M_3$, $ M_2M_4$, $ M_2\phi_1^2$, $ M_1^2$, $ M_1M_3$, $ M_3^2$, $ M_1M_4$, $ M_3M_4$, $ M_4^2$, $ M_1\phi_1^2$, $ M_3\phi_1^2$, $ M_4\phi_1^2$, $ \phi_1^4$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_1q_2$, $ q_2\tilde{q}_1$, $ M_3q_1\tilde{q}_2$, $ M_4q_1\tilde{q}_2$, $ \phi_1^2q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_1^2\tilde{q}_2^2$, $ M_2q_2\tilde{q}_2$, $ M_2\phi_1\tilde{q}_2^2$, $ \phi_1q_2^2$, $ M_3q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_1\phi_1\tilde{q}_2^2$, $ M_3\phi_1\tilde{q}_2^2$, $ M_4\phi_1\tilde{q}_2^2$, $ \phi_1^3\tilde{q}_2^2$ | . | -4 | t^2.06 + 4*t^2.09 + t^2.87 + 2*t^3.89 + t^3.94 + t^4.12 + 4*t^4.15 + 10*t^4.17 + t^4.93 + 5*t^4.96 + t^5.74 + 2*t^5.94 + 6*t^5.97 - 4*t^6. + 2*t^6.03 + t^6.18 + 4*t^6.21 + 10*t^6.23 + 20*t^6.26 + 2*t^6.75 + t^6.81 + t^6.99 + 3*t^7.02 + 10*t^7.04 - 2*t^7.07 + 3*t^7.77 - t^7.8 + 2*t^7.83 - 2*t^7.85 + t^7.88 + 2*t^8. + 6*t^8.03 + 8*t^8.06 - 17*t^8.09 + 2*t^8.11 + t^8.24 + 4*t^8.27 + 10*t^8.29 + 20*t^8.32 + 35*t^8.35 + t^8.61 + 2*t^8.81 + 6*t^8.84 - 8*t^8.87 + t^8.9 - t^4.04/y - t^6.1/y - (4*t^6.13)/y + (4*t^7.15)/y + (6*t^7.17)/y + t^7.93/y + (8*t^7.96)/y + t^7.98/y - t^8.16/y - (4*t^8.19)/y - (10*t^8.22)/y + (2*t^8.94)/y + (8*t^8.97)/y - t^4.04*y - t^6.1*y - 4*t^6.13*y + 4*t^7.15*y + 6*t^7.17*y + t^7.93*y + 8*t^7.96*y + t^7.98*y - t^8.16*y - 4*t^8.19*y - 10*t^8.22*y + 2*t^8.94*y + 8*t^8.97*y | t^2.06/(g1^5*g2) + (4*t^2.09)/(g1^2*g2^2) + g1^3*g2^3*t^2.87 + (2*g2^3*t^3.89)/g1 + g1^5*g2*t^3.94 + t^4.12/(g1^10*g2^2) + (4*t^4.15)/(g1^7*g2^3) + (10*t^4.17)/(g1^4*g2^4) + (g2^2*t^4.93)/g1^2 + 5*g1*g2*t^4.96 + g1^6*g2^6*t^5.74 + (2*g2^2*t^5.94)/g1^6 + (6*g2*t^5.97)/g1^3 - 4*t^6. + (2*g1^3*t^6.03)/g2 + t^6.18/(g1^15*g2^3) + (4*t^6.21)/(g1^12*g2^4) + (10*t^6.23)/(g1^9*g2^5) + (20*t^6.26)/(g1^6*g2^6) + 2*g1^2*g2^6*t^6.75 + g1^8*g2^4*t^6.81 + (g2*t^6.99)/g1^7 + (3*t^7.02)/g1^4 + (10*t^7.04)/(g1*g2) - (2*g1^2*t^7.07)/g2^2 + (3*g2^6*t^7.77)/g1^2 - g1*g2^5*t^7.8 + 2*g1^4*g2^4*t^7.83 - 2*g1^7*g2^3*t^7.85 + g1^10*g2^2*t^7.88 + (2*g2*t^8.)/g1^11 + (6*t^8.03)/g1^8 + (8*t^8.06)/(g1^5*g2) - (17*t^8.09)/(g1^2*g2^2) + (2*g1*t^8.11)/g2^3 + t^8.24/(g1^20*g2^4) + (4*t^8.27)/(g1^17*g2^5) + (10*t^8.29)/(g1^14*g2^6) + (20*t^8.32)/(g1^11*g2^7) + (35*t^8.35)/(g1^8*g2^8) + g1^9*g2^9*t^8.61 + (2*g2^5*t^8.81)/g1^3 + 6*g2^4*t^8.84 - 8*g1^3*g2^3*t^8.87 + g1^6*g2^2*t^8.9 - t^4.04/(g1*g2*y) - t^6.1/(g1^6*g2^2*y) - (4*t^6.13)/(g1^3*g2^3*y) + (4*t^7.15)/(g1^7*g2^3*y) + (6*t^7.17)/(g1^4*g2^4*y) + (g2^2*t^7.93)/(g1^2*y) + (8*g1*g2*t^7.96)/y + (g1^4*t^7.98)/y - t^8.16/(g1^11*g2^3*y) - (4*t^8.19)/(g1^8*g2^4*y) - (10*t^8.22)/(g1^5*g2^5*y) + (2*g2^2*t^8.94)/(g1^6*y) + (8*g2*t^8.97)/(g1^3*y) - (t^4.04*y)/(g1*g2) - (t^6.1*y)/(g1^6*g2^2) - (4*t^6.13*y)/(g1^3*g2^3) + (4*t^7.15*y)/(g1^7*g2^3) + (6*t^7.17*y)/(g1^4*g2^4) + (g2^2*t^7.93*y)/g1^2 + 8*g1*g2*t^7.96*y + g1^4*t^7.98*y - (t^8.16*y)/(g1^11*g2^3) - (4*t^8.19*y)/(g1^8*g2^4) - (10*t^8.22*y)/(g1^5*g2^5) + (2*g2^2*t^8.94*y)/g1^6 + (8*g2*t^8.97*y)/g1^3 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 45986 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_2\tilde{q}_1$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ | 0.669 | 0.8353 | 0.8009 | [X:[], M:[0.6994, 0.6891, 0.6994], q:[0.4806, 0.82], qb:[0.8303, 0.4703], phi:[0.3497]] | t^2.07 + 3*t^2.1 + t^2.85 + 2*t^3.87 + t^3.9 + t^3.93 + t^4.13 + 3*t^4.17 + 6*t^4.2 + t^4.92 + 4*t^4.95 + t^5.71 + 2*t^5.94 + 5*t^5.97 - t^6. - t^4.05/y - t^4.05*y | detail |