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 |
|---|---|---|---|---|---|---|---|---|---|
| 3039 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_1M_3$ + $ M_4\phi_1\tilde{q}_1^2$ + $ M_1M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1q_2$ + $ M_7q_1\tilde{q}_1$ | 0.7001 | 0.8939 | 0.7832 | [X:[], M:[1.1194, 0.7295, 0.8806, 0.8806, 0.7295, 0.6792, 0.8302], q:[0.805, 0.5158], qb:[0.3648, 0.7547], phi:[0.3899]] | [X:[], M:[[16], [14], [-16], [-16], [14], [24], [-6]], q:[[-1], [-23]], qb:[[7], [9]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_6$, $ M_2$, $ M_5$, $ \phi_1^2$, $ M_7$, $ M_3$, $ M_4$, $ M_1$, $ M_6^2$, $ M_2M_6$, $ M_5M_6$, $ \phi_1q_2^2$, $ M_2^2$, $ M_2M_5$, $ M_5^2$, $ M_6\phi_1^2$, $ M_6M_7$, $ M_2\phi_1^2$, $ M_5\phi_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3M_6$, $ M_4M_6$, $ M_2M_7$, $ M_5M_7$, $ \phi_1^4$, $ q_1\tilde{q}_2$, $ M_2M_3$, $ M_2M_4$, $ M_3M_5$, $ M_4M_5$, $ M_7\phi_1^2$, $ M_7^2$, $ M_3\phi_1^2$, $ M_4\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_3M_7$, $ M_4M_7$, $ M_3^2$, $ M_3M_4$, $ M_4^2$, $ M_1M_6$, $ M_1M_2$, $ M_1M_5$, $ M_1\phi_1^2$, $ \phi_1\tilde{q}_2^2$ | . | -2 | t^2.04 + 2*t^2.19 + t^2.34 + t^2.49 + 2*t^2.64 + t^3.36 + t^4.08 + 2*t^4.23 + t^4.26 + 4*t^4.38 + 4*t^4.53 + 6*t^4.68 + 4*t^4.83 + 4*t^4.98 + 2*t^5.13 + 2*t^5.28 + t^5.4 + t^5.55 + 2*t^5.7 - 2*t^6. + t^6.11 - t^6.15 + 2*t^6.26 + 4*t^6.41 + 8*t^6.57 + t^6.6 + 10*t^6.72 + t^6.76 + 11*t^6.87 + 2*t^6.91 + 11*t^7.02 + 9*t^7.17 + 8*t^7.32 + t^7.43 + 6*t^7.47 + t^7.58 + 4*t^7.62 + 3*t^7.74 + t^7.77 + 3*t^7.89 + t^7.92 - t^8.04 + t^8.15 - 7*t^8.19 + 2*t^8.3 - 5*t^8.34 + 4*t^8.45 - 8*t^8.49 + t^8.53 + 8*t^8.6 - 7*t^8.64 + 15*t^8.75 - 2*t^8.79 + 16*t^8.91 + t^8.94 - t^4.17/y - t^6.21/y - (2*t^6.36)/y - t^6.51/y - t^6.66/y - t^6.81/y + (2*t^7.23)/y + (2*t^7.38)/y + (4*t^7.53)/y + (5*t^7.68)/y + (6*t^7.83)/y + (4*t^7.98)/y + (3*t^8.13)/y - t^8.24/y + t^8.28/y - t^8.4/y - (2*t^8.55)/y - (2*t^8.7)/y - (3*t^8.85)/y - t^4.17*y - t^6.21*y - 2*t^6.36*y - t^6.51*y - t^6.66*y - t^6.81*y + 2*t^7.23*y + 2*t^7.38*y + 4*t^7.53*y + 5*t^7.68*y + 6*t^7.83*y + 4*t^7.98*y + 3*t^8.13*y - t^8.24*y + t^8.28*y - t^8.4*y - 2*t^8.55*y - 2*t^8.7*y - 3*t^8.85*y | g1^24*t^2.04 + 2*g1^14*t^2.19 + g1^4*t^2.34 + t^2.49/g1^6 + (2*t^2.64)/g1^16 + g1^16*t^3.36 + g1^48*t^4.08 + 2*g1^38*t^4.23 + t^4.26/g1^44 + 4*g1^28*t^4.38 + 4*g1^18*t^4.53 + 6*g1^8*t^4.68 + (4*t^4.83)/g1^2 + (4*t^4.98)/g1^12 + (2*t^5.13)/g1^22 + (2*t^5.28)/g1^32 + g1^40*t^5.4 + g1^30*t^5.55 + 2*g1^20*t^5.7 - 2*t^6. + g1^72*t^6.11 - t^6.15/g1^10 + 2*g1^62*t^6.26 + 4*g1^52*t^6.41 + 8*g1^42*t^6.57 + t^6.6/g1^40 + 10*g1^32*t^6.72 + t^6.76/g1^50 + 11*g1^22*t^6.87 + (2*t^6.91)/g1^60 + 11*g1^12*t^7.02 + 9*g1^2*t^7.17 + (8*t^7.32)/g1^8 + g1^64*t^7.43 + (6*t^7.47)/g1^18 + g1^54*t^7.58 + (4*t^7.62)/g1^28 + 3*g1^44*t^7.74 + t^7.77/g1^38 + 3*g1^34*t^7.89 + t^7.92/g1^48 - g1^24*t^8.04 + g1^96*t^8.15 - 7*g1^14*t^8.19 + 2*g1^86*t^8.3 - 5*g1^4*t^8.34 + 4*g1^76*t^8.45 - (8*t^8.49)/g1^6 + t^8.53/g1^88 + 8*g1^66*t^8.6 - (7*t^8.64)/g1^16 + 15*g1^56*t^8.75 - (2*t^8.79)/g1^26 + 16*g1^46*t^8.91 + t^8.94/g1^36 - (g1^2*t^4.17)/y - (g1^26*t^6.21)/y - (2*g1^16*t^6.36)/y - (g1^6*t^6.51)/y - t^6.66/(g1^4*y) - t^6.81/(g1^14*y) + (2*g1^38*t^7.23)/y + (2*g1^28*t^7.38)/y + (4*g1^18*t^7.53)/y + (5*g1^8*t^7.68)/y + (6*t^7.83)/(g1^2*y) + (4*t^7.98)/(g1^12*y) + (3*t^8.13)/(g1^22*y) - (g1^50*t^8.24)/y + t^8.28/(g1^32*y) - (g1^40*t^8.4)/y - (2*g1^30*t^8.55)/y - (2*g1^20*t^8.7)/y - (3*g1^10*t^8.85)/y - g1^2*t^4.17*y - g1^26*t^6.21*y - 2*g1^16*t^6.36*y - g1^6*t^6.51*y - (t^6.66*y)/g1^4 - (t^6.81*y)/g1^14 + 2*g1^38*t^7.23*y + 2*g1^28*t^7.38*y + 4*g1^18*t^7.53*y + 5*g1^8*t^7.68*y + (6*t^7.83*y)/g1^2 + (4*t^7.98*y)/g1^12 + (3*t^8.13*y)/g1^22 - g1^50*t^8.24*y + (t^8.28*y)/g1^32 - g1^40*t^8.4*y - 2*g1^30*t^8.55*y - 2*g1^20*t^8.7*y - 3*g1^10*t^8.85*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1983 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_1M_3$ + $ M_4\phi_1\tilde{q}_1^2$ + $ M_1M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1q_2$ | 0.6856 | 0.8692 | 0.7888 | [X:[], M:[1.1153, 0.7259, 0.8847, 0.8847, 0.7259, 0.6729], q:[0.8053, 0.5218], qb:[0.3629, 0.7523], phi:[0.3894]] | t^2.02 + 2*t^2.18 + t^2.34 + 2*t^2.65 + t^3.35 + t^3.5 + t^4.04 + 2*t^4.2 + t^4.3 + 4*t^4.36 + 3*t^4.51 + 4*t^4.67 + 3*t^4.83 + 3*t^4.99 + 2*t^5.31 + t^5.36 + 2*t^5.52 + 4*t^5.68 - 2*t^6. - t^4.17/y - t^4.17*y | detail |