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 |
|---|---|---|---|---|---|---|---|---|---|
| 46589 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_2q_1q_2$ + $ M_3\phi_1q_2\tilde{q}_1$ + $ M_4q_1\tilde{q}_2$ | 0.6668 | 0.8608 | 0.7747 | [X:[], M:[1.1031, 0.7937, 0.6906, 0.8094], q:[0.75, 0.4563], qb:[0.3531, 0.4406], phi:[0.5]] | [X:[], M:[[-1], [2], [3], [-3]], q:[[0], [-2]], qb:[[-1], [3]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ M_2$, $ \tilde{q}_1\tilde{q}_2$, $ M_4$, $ q_2\tilde{q}_1$, $ \phi_1^2$, $ M_1$, $ q_1\tilde{q}_1$, $ q_1q_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ M_2M_3$, $ M_3\tilde{q}_1\tilde{q}_2$, $ M_3M_4$, $ M_3q_2\tilde{q}_1$, $ M_2^2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_2M_4$, $ M_2q_2\tilde{q}_1$, $ M_4\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_4^2$, $ M_4q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_3\phi_1^2$, $ M_1M_3$, $ M_2\phi_1^2$, $ M_3q_1\tilde{q}_1$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ M_4\phi_1^2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_1M_2$, $ M_3q_1q_2$, $ M_2q_1\tilde{q}_1$, $ q_1\tilde{q}_1^2\tilde{q}_2$, $ M_1M_4$, $ M_4q_1\tilde{q}_1$, $ q_1q_2\tilde{q}_1^2$ | . | -1 | t^2.07 + 2*t^2.38 + 2*t^2.43 + t^3. + 2*t^3.31 + t^3.62 + t^3.88 + 2*t^4.14 + t^4.19 + t^4.24 + 2*t^4.45 + 2*t^4.5 + 3*t^4.76 + 4*t^4.81 + 3*t^4.86 + t^5.07 + 4*t^5.38 + 2*t^5.43 + 4*t^5.69 + 3*t^5.74 - t^6. + t^6.05 + 2*t^6.22 + 2*t^6.26 + 2*t^6.31 + 4*t^6.52 + 4*t^6.57 + 5*t^6.62 + 2*t^6.67 + 3*t^6.83 + 3*t^6.88 + 3*t^6.93 + 5*t^7.14 + 5*t^7.19 + 5*t^7.24 + 4*t^7.28 + 4*t^7.45 + t^7.5 + 6*t^7.76 + 4*t^7.81 + 3*t^7.86 + t^8.02 + 2*t^8.07 + 4*t^8.12 + 4*t^8.17 + 3*t^8.29 + t^8.33 - 2*t^8.38 - 3*t^8.43 + 2*t^8.48 + 4*t^8.6 + 5*t^8.64 + 4*t^8.69 + 2*t^8.74 + 6*t^8.91 + 5*t^8.95 - t^4.5/y - t^6.57/y - t^6.88/y - t^6.93/y + t^7.19/y + (2*t^7.45)/y + (2*t^7.5)/y + t^7.76/y + (3*t^7.81)/y + t^7.86/y + (2*t^8.07)/y + t^8.12/y + (4*t^8.38)/y + (3*t^8.43)/y - t^8.64/y + (5*t^8.69)/y + (4*t^8.74)/y - t^4.5*y - t^6.57*y - t^6.88*y - t^6.93*y + t^7.19*y + 2*t^7.45*y + 2*t^7.5*y + t^7.76*y + 3*t^7.81*y + t^7.86*y + 2*t^8.07*y + t^8.12*y + 4*t^8.38*y + 3*t^8.43*y - t^8.64*y + 5*t^8.69*y + 4*t^8.74*y | g1^3*t^2.07 + 2*g1^2*t^2.38 + (2*t^2.43)/g1^3 + t^3. + (2*t^3.31)/g1 + t^3.62/g1^2 + g1^2*t^3.88 + 2*g1^6*t^4.14 + g1*t^4.19 + t^4.24/g1^4 + 2*g1^5*t^4.45 + 2*t^4.5 + 3*g1^4*t^4.76 + (4*t^4.81)/g1 + (3*t^4.86)/g1^6 + g1^3*t^5.07 + 4*g1^2*t^5.38 + (2*t^5.43)/g1^3 + 4*g1*t^5.69 + (3*t^5.74)/g1^4 - t^6. + t^6.05/g1^5 + 2*g1^9*t^6.22 + 2*g1^4*t^6.26 + (2*t^6.31)/g1 + 4*g1^8*t^6.52 + 4*g1^3*t^6.57 + (5*t^6.62)/g1^2 + (2*t^6.67)/g1^7 + 3*g1^7*t^6.83 + 3*g1^2*t^6.88 + (3*t^6.93)/g1^3 + 5*g1^6*t^7.14 + 5*g1*t^7.19 + (5*t^7.24)/g1^4 + (4*t^7.28)/g1^9 + 4*g1^5*t^7.45 + t^7.5 + 6*g1^4*t^7.76 + (4*t^7.81)/g1 + (3*t^7.86)/g1^6 + g1^8*t^8.02 + 2*g1^3*t^8.07 + (4*t^8.12)/g1^2 + (4*t^8.17)/g1^7 + 3*g1^12*t^8.29 + g1^7*t^8.33 - 2*g1^2*t^8.38 - (3*t^8.43)/g1^3 + (2*t^8.48)/g1^8 + 4*g1^11*t^8.6 + 5*g1^6*t^8.64 + 4*g1*t^8.69 + (2*t^8.74)/g1^4 + 6*g1^10*t^8.91 + 5*g1^5*t^8.95 - t^4.5/y - (g1^3*t^6.57)/y - (g1^2*t^6.88)/y - t^6.93/(g1^3*y) + (g1*t^7.19)/y + (2*g1^5*t^7.45)/y + (2*t^7.5)/y + (g1^4*t^7.76)/y + (3*t^7.81)/(g1*y) + t^7.86/(g1^6*y) + (2*g1^3*t^8.07)/y + t^8.12/(g1^2*y) + (4*g1^2*t^8.38)/y + (3*t^8.43)/(g1^3*y) - (g1^6*t^8.64)/y + (5*g1*t^8.69)/y + (4*t^8.74)/(g1^4*y) - t^4.5*y - g1^3*t^6.57*y - g1^2*t^6.88*y - (t^6.93*y)/g1^3 + g1*t^7.19*y + 2*g1^5*t^7.45*y + 2*t^7.5*y + g1^4*t^7.76*y + (3*t^7.81*y)/g1 + (t^7.86*y)/g1^6 + 2*g1^3*t^8.07*y + (t^8.12*y)/g1^2 + 4*g1^2*t^8.38*y + (3*t^8.43*y)/g1^3 - g1^6*t^8.64*y + 5*g1*t^8.69*y + (4*t^8.74*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46232 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_2q_1q_2$ + $ M_3\phi_1q_2\tilde{q}_1$ | 0.6515 | 0.8349 | 0.7802 | [X:[], M:[1.1089, 0.7822, 0.6732], q:[0.75, 0.4678], qb:[0.3589, 0.4232], phi:[0.5]] | t^2.02 + 2*t^2.35 + t^2.48 + t^3. + 2*t^3.33 + t^3.52 + t^3.65 + t^3.85 + 2*t^4.04 + t^4.17 + t^4.31 + 2*t^4.37 + t^4.5 + 3*t^4.69 + 2*t^4.83 + t^4.96 + t^5.02 + 4*t^5.35 + t^5.48 + t^5.54 + 4*t^5.67 + t^5.81 + 2*t^5.87 - t^4.5/y - t^4.5*y | detail |