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 |
|---|---|---|---|---|---|---|---|---|---|
| 4466 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_2^2$ + $ M_4q_2\tilde{q}_2$ + $ M_1X_1$ + $ M_2M_5$ + $ M_6\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_7q_1\tilde{q}_2$ + $ M_8q_1\tilde{q}_1$ | 0.6847 | 0.8722 | 0.785 | [X:[1.5666], M:[0.4334, 1.1889, 0.7833, 0.8668, 0.8111, 0.7833, 0.839, 0.7555], q:[0.7972, 0.7694], qb:[0.4473, 0.3638], phi:[0.4056]] | [X:[[12]], M:[[-12], [4], [6], [-24], [-4], [6], [-14], [16]], q:[[1], [11]], qb:[[-17], [13]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_8$, $ M_3$, $ M_6$, $ M_5$, $ \phi_1^2$, $ M_7$, $ M_4$, $ q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ M_8^2$, $ M_3M_8$, $ M_6M_8$, $ \phi_1q_2\tilde{q}_2$, $ M_3^2$, $ M_3M_6$, $ M_6^2$, $ M_5M_8$, $ M_8\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ X_1$, $ M_3M_5$, $ M_5M_6$, $ M_7M_8$, $ M_3\phi_1^2$, $ M_6\phi_1^2$, $ M_5^2$, $ M_3M_7$, $ M_6M_7$, $ M_4M_8$, $ M_5\phi_1^2$, $ \phi_1^4$, $ \phi_1q_2\tilde{q}_1$, $ M_3M_4$, $ M_4M_6$, $ M_5M_7$, $ M_7\phi_1^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4M_5$, $ M_7^2$, $ M_4\phi_1^2$, $ M_4M_7$, $ M_4^2$, $ M_8q_2\tilde{q}_2$, $ M_3q_2\tilde{q}_2$, $ M_6q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ M_5q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$ | . | -3 | t^2.27 + 2*t^2.35 + 2*t^2.43 + t^2.52 + t^2.6 + t^3.4 + t^3.9 + t^4.53 + 3*t^4.62 + 6*t^4.7 + 4*t^4.78 + 7*t^4.87 + 4*t^4.95 + 2*t^5.03 + t^5.12 + t^5.2 + t^5.67 + t^5.75 + 3*t^5.83 - 3*t^6. - t^6.08 + 2*t^6.33 + t^6.42 + t^6.5 + 2*t^6.8 + 3*t^6.88 + 5*t^6.97 + 10*t^7.05 + 11*t^7.13 + 11*t^7.22 + 13*t^7.3 + 8*t^7.38 + 5*t^7.47 + 4*t^7.55 + 2*t^7.63 + t^7.72 + 2*t^7.8 + t^7.93 + 2*t^8.02 + 4*t^8.1 + t^8.18 - t^8.27 - 8*t^8.35 - 9*t^8.43 - 7*t^8.52 - 4*t^8.6 - t^8.68 + 4*t^8.77 + 2*t^8.85 + 2*t^8.93 - t^4.22/y - t^6.48/y - (2*t^6.57)/y - t^6.65/y - t^6.73/y - t^6.82/y + (3*t^7.62)/y + (4*t^7.7)/y + (6*t^7.78)/y + (6*t^7.87)/y + (5*t^7.95)/y + (2*t^8.03)/y + t^8.12/y + t^8.67/y + t^8.75/y - (3*t^8.92)/y - t^4.22*y - t^6.48*y - 2*t^6.57*y - t^6.65*y - t^6.73*y - t^6.82*y + 3*t^7.62*y + 4*t^7.7*y + 6*t^7.78*y + 6*t^7.87*y + 5*t^7.95*y + 2*t^8.03*y + t^8.12*y + t^8.67*y + t^8.75*y - 3*t^8.92*y | g1^16*t^2.27 + 2*g1^6*t^2.35 + (2*t^2.43)/g1^4 + t^2.52/g1^14 + t^2.6/g1^24 + g1^24*t^3.4 + t^3.9/g1^36 + g1^32*t^4.53 + 3*g1^22*t^4.62 + 6*g1^12*t^4.7 + 4*g1^2*t^4.78 + (7*t^4.87)/g1^8 + (4*t^4.95)/g1^18 + (2*t^5.03)/g1^28 + t^5.12/g1^38 + t^5.2/g1^48 + g1^40*t^5.67 + g1^30*t^5.75 + 3*g1^20*t^5.83 - 3*t^6. - t^6.08/g1^10 + (2*t^6.33)/g1^40 + t^6.42/g1^50 + t^6.5/g1^60 + 2*g1^48*t^6.8 + 3*g1^38*t^6.88 + 5*g1^28*t^6.97 + 10*g1^18*t^7.05 + 11*g1^8*t^7.13 + (11*t^7.22)/g1^2 + (13*t^7.3)/g1^12 + (8*t^7.38)/g1^22 + (5*t^7.47)/g1^32 + (4*t^7.55)/g1^42 + (2*t^7.63)/g1^52 + t^7.72/g1^62 + (2*t^7.8)/g1^72 + g1^56*t^7.93 + 2*g1^46*t^8.02 + 4*g1^36*t^8.1 + g1^26*t^8.18 - g1^16*t^8.27 - 8*g1^6*t^8.35 - (9*t^8.43)/g1^4 - (7*t^8.52)/g1^14 - (4*t^8.6)/g1^24 - t^8.68/g1^34 + (4*t^8.77)/g1^44 + (2*t^8.85)/g1^54 + (2*t^8.93)/g1^64 - t^4.22/(g1^2*y) - (g1^14*t^6.48)/y - (2*g1^4*t^6.57)/y - t^6.65/(g1^6*y) - t^6.73/(g1^16*y) - t^6.82/(g1^26*y) + (3*g1^22*t^7.62)/y + (4*g1^12*t^7.7)/y + (6*g1^2*t^7.78)/y + (6*t^7.87)/(g1^8*y) + (5*t^7.95)/(g1^18*y) + (2*t^8.03)/(g1^28*y) + t^8.12/(g1^38*y) + (g1^40*t^8.67)/y + (g1^30*t^8.75)/y - (3*g1^10*t^8.92)/y - (t^4.22*y)/g1^2 - g1^14*t^6.48*y - 2*g1^4*t^6.57*y - (t^6.65*y)/g1^6 - (t^6.73*y)/g1^16 - (t^6.82*y)/g1^26 + 3*g1^22*t^7.62*y + 4*g1^12*t^7.7*y + 6*g1^2*t^7.78*y + (6*t^7.87*y)/g1^8 + (5*t^7.95*y)/g1^18 + (2*t^8.03*y)/g1^28 + (t^8.12*y)/g1^38 + g1^40*t^8.67*y + g1^30*t^8.75*y - 3*g1^10*t^8.92*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2423 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_2^2$ + $ M_4q_2\tilde{q}_2$ + $ M_1X_1$ + $ M_2M_5$ + $ M_6\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_7q_1\tilde{q}_2$ | 0.6661 | 0.8389 | 0.794 | [X:[1.5734], M:[0.4266, 1.1911, 0.7867, 0.8532, 0.8089, 0.7867, 0.8311], q:[0.7978, 0.7756], qb:[0.4377, 0.3712], phi:[0.4044]] | 2*t^2.36 + 2*t^2.43 + t^2.49 + t^2.56 + t^3.44 + t^3.71 + t^3.84 + t^4.65 + 4*t^4.72 + 3*t^4.79 + 6*t^4.85 + 4*t^4.92 + 2*t^4.99 + t^5.05 + t^5.12 + t^5.8 + 3*t^5.87 - 3*t^6. - t^4.21/y - t^4.21*y | detail |