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 |
|---|---|---|---|---|---|---|---|---|---|
| 46397 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_4\phi_1q_2^2$ | 0.6147 | 0.7919 | 0.7762 | [X:[], M:[0.9688, 1.0312, 0.8358, 0.9064], q:[0.7422, 0.289], qb:[0.4844, 0.422], phi:[0.5156]] | [X:[], M:[[4], [-4], [-11], [12]], q:[[1], [-5]], qb:[[2], [10]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ M_3$, $ M_4$, $ \tilde{q}_1\tilde{q}_2$, $ M_2$, $ \phi_1^2$, $ q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ \phi_1q_1q_2$, $ q_2^2\tilde{q}_1^2$, $ M_3q_2\tilde{q}_2$, $ M_3q_2\tilde{q}_1$, $ M_4q_2\tilde{q}_2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_3^2$, $ M_4q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_3M_4$, $ \phi_1q_1\tilde{q}_1$, $ M_2q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ M_2q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_4^2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_2M_3$, $ M_3\phi_1^2$, $ M_2M_4$, $ M_4\phi_1^2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_2^2$ | $\phi_1q_2^2\tilde{q}_1\tilde{q}_2$ | -1 | t^2.13 + t^2.32 + t^2.51 + 2*t^2.72 + 2*t^3.09 + 2*t^3.68 + t^3.87 + t^4.08 + 2*t^4.27 + 2*t^4.45 + 2*t^4.64 + t^4.83 + 2*t^4.85 + t^5.01 + 2*t^5.04 + 4*t^5.23 + t^5.41 + 3*t^5.44 + t^5.6 + 4*t^5.81 - t^6. + 3*t^6.19 + t^6.21 + t^6.37 + 5*t^6.4 + 2*t^6.59 + 4*t^6.77 + 2*t^6.8 + 2*t^6.96 + 3*t^6.99 + t^7.15 + 4*t^7.17 + t^7.33 + 5*t^7.36 + t^7.52 + 2*t^7.55 + 3*t^7.57 + 3*t^7.73 + 4*t^7.76 + 6*t^7.95 + t^8.11 - t^8.13 + 5*t^8.16 + 2*t^8.32 + 2*t^8.35 - 2*t^8.51 + 8*t^8.53 + t^8.69 - 2*t^8.72 + t^8.88 + 5*t^8.91 + 2*t^8.93 - t^4.55/y - t^7.05/y - t^7.27/y + (2*t^7.45)/y + (2*t^7.83)/y + (2*t^7.85)/y + (3*t^8.04)/y + (4*t^8.23)/y + (2*t^8.41)/y + t^8.44/y + (2*t^8.6)/y + (6*t^8.81)/y - t^4.55*y - t^7.05*y - t^7.27*y + 2*t^7.45*y + 2*t^7.83*y + 2*t^7.85*y + 3*t^8.04*y + 4*t^8.23*y + 2*t^8.41*y + t^8.44*y + 2*t^8.6*y + 6*t^8.81*y | g1^5*t^2.13 + t^2.32/g1^3 + t^2.51/g1^11 + 2*g1^12*t^2.72 + (2*t^3.09)/g1^4 + 2*g1^3*t^3.68 + t^3.87/g1^5 + g1^18*t^4.08 + 2*g1^10*t^4.27 + 2*g1^2*t^4.45 + (2*t^4.64)/g1^6 + t^4.83/g1^14 + 2*g1^17*t^4.85 + t^5.01/g1^22 + 2*g1^9*t^5.04 + 4*g1*t^5.23 + t^5.41/g1^7 + 3*g1^24*t^5.44 + t^5.6/g1^15 + 4*g1^8*t^5.81 - t^6. + (3*t^6.19)/g1^8 + g1^23*t^6.21 + t^6.37/g1^16 + 5*g1^15*t^6.4 + 2*g1^7*t^6.59 + (4*t^6.77)/g1 + 2*g1^30*t^6.8 + (2*t^6.96)/g1^9 + 3*g1^22*t^6.99 + t^7.15/g1^17 + 4*g1^14*t^7.17 + t^7.33/g1^25 + 5*g1^6*t^7.36 + t^7.52/g1^33 + (2*t^7.55)/g1^2 + 3*g1^29*t^7.57 + (3*t^7.73)/g1^10 + 4*g1^21*t^7.76 + 6*g1^13*t^7.95 + t^8.11/g1^26 - g1^5*t^8.13 + 5*g1^36*t^8.16 + (2*t^8.32)/g1^3 + 2*g1^28*t^8.35 - (2*t^8.51)/g1^11 + 8*g1^20*t^8.53 + t^8.69/g1^19 - 2*g1^12*t^8.72 + t^8.88/g1^27 + 5*g1^4*t^8.91 + 2*g1^35*t^8.93 - t^4.55/(g1^2*y) - t^7.05/(g1^13*y) - (g1^10*t^7.27)/y + (2*g1^2*t^7.45)/y + (2*t^7.83)/(g1^14*y) + (2*g1^17*t^7.85)/y + (3*g1^9*t^8.04)/y + (4*g1*t^8.23)/y + (2*t^8.41)/(g1^7*y) + (g1^24*t^8.44)/y + (2*t^8.6)/(g1^15*y) + (6*g1^8*t^8.81)/y - (t^4.55*y)/g1^2 - (t^7.05*y)/g1^13 - g1^10*t^7.27*y + 2*g1^2*t^7.45*y + (2*t^7.83*y)/g1^14 + 2*g1^17*t^7.85*y + 3*g1^9*t^8.04*y + 4*g1*t^8.23*y + (2*t^8.41*y)/g1^7 + g1^24*t^8.44*y + (2*t^8.6*y)/g1^15 + 6*g1^8*t^8.81*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46173 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_3q_1\tilde{q}_2$ | 0.6079 | 0.7795 | 0.7799 | [X:[], M:[0.9824, 1.0176, 0.7984], q:[0.7456, 0.272], qb:[0.4912, 0.456], phi:[0.5088]] | t^2.18 + t^2.29 + t^2.4 + t^2.84 + 2*t^3.05 + t^3.16 + 2*t^3.71 + t^3.82 + t^4.26 + 2*t^4.37 + 2*t^4.47 + 2*t^4.58 + t^4.68 + t^4.79 + t^5.03 + t^5.13 + 3*t^5.24 + 2*t^5.34 + 2*t^5.45 + t^5.55 + t^5.68 + 2*t^5.89 - t^4.53/y - t^4.53*y | detail |