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 |
|---|---|---|---|---|---|---|---|---|---|
| 3114 | 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_5\phi_1\tilde{q}_1^2$ + $ M_6q_1\tilde{q}_2$ + $ M_7q_2\tilde{q}_2$ | 0.666 | 0.8404 | 0.7925 | [X:[1.5789], M:[0.4211, 1.193, 0.7894, 0.8423, 0.7366, 0.8247, 0.8423], q:[0.7982, 0.7806], qb:[0.4299, 0.3771], phi:[0.4035]] | [X:[[12]], M:[[-12], [4], [6], [-24], [36], [-14], [-24]], q:[[1], [11]], qb:[[-17], [13]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ M_3$, $ \phi_1^2$, $ M_6$, $ M_4$, $ M_7$, $ M_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_1$, $ M_5^2$, $ M_3M_5$, $ M_5\phi_1^2$, $ M_5M_6$, $ \phi_1q_2\tilde{q}_2$, $ M_3^2$, $ M_4M_5$, $ M_5M_7$, $ \phi_1q_1\tilde{q}_2$, $ X_1$, $ M_3M_6$, $ \phi_1^4$, $ \phi_1q_2\tilde{q}_1$, $ M_3M_4$, $ M_3M_7$, $ M_6\phi_1^2$, $ \phi_1q_1\tilde{q}_1$, $ M_6^2$, $ M_4\phi_1^2$, $ M_7\phi_1^2$, $ M_4M_6$, $ M_6M_7$, $ M_4^2$, $ M_4M_7$, $ M_7^2$, $ M_2M_5$, $ \phi_1q_2^2$, $ M_5q_1\tilde{q}_1$ | $M_3\phi_1\tilde{q}_1\tilde{q}_2$ | -2 | t^2.21 + t^2.37 + t^2.42 + t^2.47 + 2*t^2.53 + t^3.58 + t^3.63 + t^3.68 + t^4.42 + t^4.58 + t^4.63 + 2*t^4.68 + 4*t^4.74 + 3*t^4.84 + 3*t^4.9 + 2*t^4.95 + 2*t^5. + 3*t^5.05 + t^5.79 + 2*t^5.89 - 2*t^6. + 2*t^6.05 + 3*t^6.11 + t^6.16 + 2*t^6.21 + t^6.63 + t^6.79 + t^6.84 + 2*t^6.89 + 4*t^6.95 + t^7.05 + 4*t^7.1 + 2*t^7.16 + 4*t^7.21 + 8*t^7.26 + 3*t^7.32 + 5*t^7.37 + 5*t^7.42 + 3*t^7.47 + 3*t^7.53 + 4*t^7.58 + t^8. + 2*t^8.1 - 4*t^8.21 + t^8.26 + 2*t^8.32 - 3*t^8.37 + 2*t^8.42 - 2*t^8.47 - 4*t^8.53 + 3*t^8.58 + 3*t^8.63 + t^8.69 + 3*t^8.74 + t^8.84 - t^4.21/y - t^6.42/y - t^6.58/y - t^6.68/y - (2*t^6.74)/y + t^7.58/y + t^7.63/y + (3*t^7.68)/y + (3*t^7.74)/y + t^7.79/y + (2*t^7.84)/y + (3*t^7.9)/y + (2*t^7.95)/y + (3*t^8.)/y + t^8.05/y - t^8.63/y + t^8.84/y - (2*t^8.95)/y - t^4.21*y - t^6.42*y - t^6.58*y - t^6.68*y - 2*t^6.74*y + t^7.58*y + t^7.63*y + 3*t^7.68*y + 3*t^7.74*y + t^7.79*y + 2*t^7.84*y + 3*t^7.9*y + 2*t^7.95*y + 3*t^8.*y + t^8.05*y - t^8.63*y + t^8.84*y - 2*t^8.95*y | g1^36*t^2.21 + g1^6*t^2.37 + t^2.42/g1^4 + t^2.47/g1^14 + (2*t^2.53)/g1^24 + g1^4*t^3.58 + t^3.63/g1^6 + t^3.68/g1^16 + g1^72*t^4.42 + g1^42*t^4.58 + g1^32*t^4.63 + 2*g1^22*t^4.68 + 4*g1^12*t^4.74 + (3*t^4.84)/g1^8 + (3*t^4.9)/g1^18 + (2*t^4.95)/g1^28 + (2*t^5.)/g1^38 + (3*t^5.05)/g1^48 + g1^40*t^5.79 + 2*g1^20*t^5.89 - 2*t^6. + (2*t^6.05)/g1^10 + (3*t^6.11)/g1^20 + t^6.16/g1^30 + (2*t^6.21)/g1^40 + g1^108*t^6.63 + g1^78*t^6.79 + g1^68*t^6.84 + 2*g1^58*t^6.89 + 4*g1^48*t^6.95 + g1^28*t^7.05 + 4*g1^18*t^7.1 + 2*g1^8*t^7.16 + (4*t^7.21)/g1^2 + (8*t^7.26)/g1^12 + (3*t^7.32)/g1^22 + (5*t^7.37)/g1^32 + (5*t^7.42)/g1^42 + (3*t^7.47)/g1^52 + (3*t^7.53)/g1^62 + (4*t^7.58)/g1^72 + g1^76*t^8. + 2*g1^56*t^8.1 - 4*g1^36*t^8.21 + g1^26*t^8.26 + 2*g1^16*t^8.32 - 3*g1^6*t^8.37 + (2*t^8.42)/g1^4 - (2*t^8.47)/g1^14 - (4*t^8.53)/g1^24 + (3*t^8.58)/g1^34 + (3*t^8.63)/g1^44 + t^8.69/g1^54 + (3*t^8.74)/g1^64 + g1^144*t^8.84 - t^4.21/(g1^2*y) - (g1^34*t^6.42)/y - (g1^4*t^6.58)/y - t^6.68/(g1^16*y) - (2*t^6.74)/(g1^26*y) + (g1^42*t^7.58)/y + (g1^32*t^7.63)/y + (3*g1^22*t^7.68)/y + (3*g1^12*t^7.74)/y + (g1^2*t^7.79)/y + (2*t^7.84)/(g1^8*y) + (3*t^7.9)/(g1^18*y) + (2*t^7.95)/(g1^28*y) + (3*t^8.)/(g1^38*y) + t^8.05/(g1^48*y) - (g1^70*t^8.63)/y + (g1^30*t^8.84)/y - (2*g1^10*t^8.95)/y - (t^4.21*y)/g1^2 - g1^34*t^6.42*y - g1^4*t^6.58*y - (t^6.68*y)/g1^16 - (2*t^6.74*y)/g1^26 + g1^42*t^7.58*y + g1^32*t^7.63*y + 3*g1^22*t^7.68*y + 3*g1^12*t^7.74*y + g1^2*t^7.79*y + (2*t^7.84*y)/g1^8 + (3*t^7.9*y)/g1^18 + (2*t^7.95*y)/g1^28 + (3*t^8.*y)/g1^38 + (t^8.05*y)/g1^48 - g1^70*t^8.63*y + g1^30*t^8.84*y - 2*g1^10*t^8.95*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2042 | 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_5\phi_1\tilde{q}_1^2$ + $ M_6q_1\tilde{q}_2$ | 0.6532 | 0.8187 | 0.7978 | [X:[1.5674], M:[0.4326, 1.1891, 0.7837, 0.8652, 0.7022, 0.838], q:[0.7973, 0.7701], qb:[0.4462, 0.3647], phi:[0.4054]] | t^2.11 + t^2.35 + t^2.43 + t^2.51 + t^2.6 + t^3.4 + t^3.57 + t^3.65 + t^3.73 + t^4.21 + t^4.46 + t^4.54 + 2*t^4.62 + 3*t^4.7 + 3*t^4.87 + 2*t^4.95 + t^5.03 + t^5.11 + t^5.19 + t^5.51 + t^5.67 + t^5.76 + 3*t^5.84 + t^5.92 - t^6. - t^4.22/y - t^4.22*y | detail |