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 |
|---|---|---|---|---|---|---|---|---|---|
| 3875 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1q_1\tilde{q}_2$ + $ M_2\phi_1q_2^2$ + $ M_5M_6$ + $ M_7\phi_1q_2^2$ | 0.6864 | 0.8761 | 0.7835 | [X:[], M:[0.7363, 0.8071, 0.7008, 0.8425, 1.1575, 0.8425, 0.8071], q:[0.8602, 0.4035], qb:[0.439, 0.754], phi:[0.3858]] | [X:[], M:[[18], [-2], [28], [-12], [12], [-12], [-2]], q:[[-17], [-1]], qb:[[-11], [13]], phi:[[4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ M_1$, $ \phi_1^2$, $ M_2$, $ M_7$, $ M_4$, $ M_6$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_3^2$, $ M_1M_3$, $ M_1^2$, $ M_3\phi_1^2$, $ M_2M_3$, $ M_3M_7$, $ M_1\phi_1^2$, $ M_1M_2$, $ M_3M_4$, $ M_3M_6$, $ M_1M_7$, $ \phi_1^4$, $ \phi_1q_2\tilde{q}_2$, $ M_1M_4$, $ M_1M_6$, $ M_2\phi_1^2$, $ M_7\phi_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2^2$, $ M_2M_7$, $ M_7^2$, $ M_4\phi_1^2$, $ M_6\phi_1^2$, $ q_1\tilde{q}_2$, $ M_2M_4$, $ M_2M_6$, $ M_4M_7$, $ M_6M_7$, $ \phi_1q_1q_2$, $ M_4^2$, $ M_4M_6$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$ | $\phi_1^3q_2\tilde{q}_1$, $ M_1\phi_1\tilde{q}_1^2$ | -1 | t^2.1 + t^2.21 + t^2.32 + 2*t^2.42 + 2*t^2.53 + t^3.68 + t^3.79 + t^4.21 + t^4.31 + 2*t^4.42 + 3*t^4.52 + 5*t^4.63 + 4*t^4.74 + 6*t^4.84 + 4*t^4.95 + 3*t^5.05 - t^6. + t^6.11 + 3*t^6.21 + t^6.31 + 2*t^6.32 + t^6.41 + 2*t^6.52 + 4*t^6.63 + 6*t^6.73 + 7*t^6.84 + 10*t^6.95 + 10*t^7.05 + 10*t^7.16 + 9*t^7.26 + 8*t^7.37 + 5*t^7.48 + 4*t^7.58 - t^8. - 3*t^8.1 - 4*t^8.21 - 4*t^8.32 + t^8.41 - 6*t^8.42 + t^8.52 - 3*t^8.53 + 2*t^8.62 + 2*t^8.63 + 4*t^8.73 + 4*t^8.74 + 7*t^8.84 + 3*t^8.85 + 8*t^8.94 - t^4.16/y - t^6.26/y - t^6.37/y - t^6.47/y - (2*t^6.58)/y - t^6.68/y + t^7.31/y + t^7.42/y + (3*t^7.52)/y + (5*t^7.63)/y + (6*t^7.74)/y + (4*t^7.84)/y + (5*t^7.95)/y + (2*t^8.05)/y - t^8.36/y - t^8.47/y - (2*t^8.58)/y - (3*t^8.68)/y - (3*t^8.79)/y - t^8.89/y - t^4.16*y - t^6.26*y - t^6.37*y - t^6.47*y - 2*t^6.58*y - t^6.68*y + t^7.31*y + t^7.42*y + 3*t^7.52*y + 5*t^7.63*y + 6*t^7.74*y + 4*t^7.84*y + 5*t^7.95*y + 2*t^8.05*y - t^8.36*y - t^8.47*y - 2*t^8.58*y - 3*t^8.68*y - 3*t^8.79*y - t^8.89*y | g1^28*t^2.1 + g1^18*t^2.21 + g1^8*t^2.32 + (2*t^2.42)/g1^2 + (2*t^2.53)/g1^12 + t^3.68/g1^8 + t^3.79/g1^18 + g1^56*t^4.21 + g1^46*t^4.31 + 2*g1^36*t^4.42 + 3*g1^26*t^4.52 + 5*g1^16*t^4.63 + 4*g1^6*t^4.74 + (6*t^4.84)/g1^4 + (4*t^4.95)/g1^14 + (3*t^5.05)/g1^24 - t^6. + t^6.11/g1^10 + (3*t^6.21)/g1^20 + g1^84*t^6.31 + (2*t^6.32)/g1^30 + g1^74*t^6.41 + 2*g1^64*t^6.52 + 4*g1^54*t^6.63 + 6*g1^44*t^6.73 + 7*g1^34*t^6.84 + 10*g1^24*t^6.95 + 10*g1^14*t^7.05 + 10*g1^4*t^7.16 + (9*t^7.26)/g1^6 + (8*t^7.37)/g1^16 + (5*t^7.48)/g1^26 + (4*t^7.58)/g1^36 - g1^38*t^8. - 3*g1^28*t^8.1 - 4*g1^18*t^8.21 - 4*g1^8*t^8.32 + g1^112*t^8.41 - (6*t^8.42)/g1^2 + g1^102*t^8.52 - (3*t^8.53)/g1^12 + 2*g1^92*t^8.62 + (2*t^8.63)/g1^22 + 4*g1^82*t^8.73 + (4*t^8.74)/g1^32 + 7*g1^72*t^8.84 + (3*t^8.85)/g1^42 + 8*g1^62*t^8.94 - (g1^4*t^4.16)/y - (g1^32*t^6.26)/y - (g1^22*t^6.37)/y - (g1^12*t^6.47)/y - (2*g1^2*t^6.58)/y - t^6.68/(g1^8*y) + (g1^46*t^7.31)/y + (g1^36*t^7.42)/y + (3*g1^26*t^7.52)/y + (5*g1^16*t^7.63)/y + (6*g1^6*t^7.74)/y + (4*t^7.84)/(g1^4*y) + (5*t^7.95)/(g1^14*y) + (2*t^8.05)/(g1^24*y) - (g1^60*t^8.36)/y - (g1^50*t^8.47)/y - (2*g1^40*t^8.58)/y - (3*g1^30*t^8.68)/y - (3*g1^20*t^8.79)/y - (g1^10*t^8.89)/y - g1^4*t^4.16*y - g1^32*t^6.26*y - g1^22*t^6.37*y - g1^12*t^6.47*y - 2*g1^2*t^6.58*y - (t^6.68*y)/g1^8 + g1^46*t^7.31*y + g1^36*t^7.42*y + 3*g1^26*t^7.52*y + 5*g1^16*t^7.63*y + 6*g1^6*t^7.74*y + (4*t^7.84*y)/g1^4 + (5*t^7.95*y)/g1^14 + (2*t^8.05*y)/g1^24 - g1^60*t^8.36*y - g1^50*t^8.47*y - 2*g1^40*t^8.58*y - 3*g1^30*t^8.68*y - 3*g1^20*t^8.79*y - g1^10*t^8.89*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 |
|---|---|---|---|---|---|---|---|---|---|
| 3392 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1q_1\tilde{q}_2$ + $ M_2\phi_1q_2^2$ + $ M_5M_6$ | 0.6704 | 0.8481 | 0.7904 | [X:[], M:[0.7343, 0.8073, 0.6978, 0.8438, 1.1562, 0.8438], q:[0.8621, 0.4037], qb:[0.4402, 0.7525], phi:[0.3854]] | t^2.09 + t^2.2 + t^2.31 + t^2.42 + 2*t^2.53 + t^3.58 + t^3.69 + t^3.8 + t^4.19 + t^4.3 + 2*t^4.41 + 2*t^4.52 + 4*t^4.62 + 3*t^4.73 + 4*t^4.84 + 2*t^4.95 + 3*t^5.06 + t^5.67 + t^5.78 + t^5.89 - t^4.16/y - t^4.16*y | detail |