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 |
|---|---|---|---|---|---|---|---|---|---|
| 3641 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_3q_1\tilde{q}_1$ + $ M_3\phi_1q_2\tilde{q}_2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_2M_5$ | 0.625 | 0.8101 | 0.7716 | [X:[], M:[1.0, 0.9607, 0.7353, 0.7549, 1.0393], q:[0.7549, 0.2451], qb:[0.5098, 0.5294], phi:[0.4902]] | [X:[], M:[[0], [-8], [-3], [1], [8]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ M_4$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ \phi_1^2$, $ \phi_1q_2^2$, $ M_1$, $ M_5$, $ \phi_1q_2\tilde{q}_2$, $ q_1\tilde{q}_2$, $ M_3^2$, $ M_3M_4$, $ \phi_1q_1q_2$, $ M_3q_2\tilde{q}_1$, $ M_4^2$, $ M_4q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ M_3q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_2^2$, $ M_3\phi_1^2$, $ M_3\phi_1q_2^2$, $ M_1M_3$, $ M_4\phi_1^2$, $ M_4\phi_1q_2^2$, $ \phi_1^2q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_1M_4$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_3M_5$, $ \phi_1q_1\tilde{q}_2$, $ M_4M_5$, $ M_5q_2\tilde{q}_1$, $ M_5q_2\tilde{q}_2$, $ \phi_1^4$, $ \phi_1^3q_2^2$, $ \phi_1^2q_2^4$ | . | -2 | t^2.21 + 2*t^2.26 + t^2.32 + 2*t^2.94 + t^3. + t^3.12 + t^3.79 + t^3.85 + t^4.41 + 2*t^4.47 + 5*t^4.53 + 3*t^4.59 + 2*t^4.65 + t^5.15 + 4*t^5.21 + 4*t^5.26 + 2*t^5.32 + 2*t^5.38 + t^5.44 + 3*t^5.88 - 2*t^6. + 3*t^6.06 + 3*t^6.12 + t^6.18 + t^6.24 + 4*t^6.74 + 8*t^6.79 + 6*t^6.85 + 5*t^6.91 + 3*t^6.97 + t^7.35 + t^7.41 + 6*t^7.47 + 6*t^7.53 + 6*t^7.59 + 6*t^7.65 + 3*t^7.71 + 2*t^7.77 + t^8.09 + 3*t^8.15 - 5*t^8.26 + 5*t^8.38 + 5*t^8.44 + 4*t^8.5 + t^8.56 + 5*t^8.82 - t^8.88 - 6*t^8.94 - t^4.47/y - t^6.68/y - t^6.74/y - t^7.41/y + (2*t^7.47)/y + (3*t^7.53)/y + (2*t^7.59)/y + (2*t^8.15)/y + (6*t^8.21)/y + (5*t^8.26)/y + (2*t^8.32)/y + (2*t^8.38)/y + t^8.44/y + t^8.94/y - t^4.47*y - t^6.68*y - t^6.74*y - t^7.41*y + 2*t^7.47*y + 3*t^7.53*y + 2*t^7.59*y + 2*t^8.15*y + 6*t^8.21*y + 5*t^8.26*y + 2*t^8.32*y + 2*t^8.38*y + t^8.44*y + t^8.94*y | t^2.21/g1^3 + 2*g1*t^2.26 + g1^5*t^2.32 + (2*t^2.94)/g1^4 + t^3. + g1^8*t^3.12 + g1^3*t^3.79 + g1^7*t^3.85 + t^4.41/g1^6 + (2*t^4.47)/g1^2 + 5*g1^2*t^4.53 + 3*g1^6*t^4.59 + 2*g1^10*t^4.65 + t^5.15/g1^7 + (4*t^5.21)/g1^3 + 4*g1*t^5.26 + 2*g1^5*t^5.32 + 2*g1^9*t^5.38 + g1^13*t^5.44 + (3*t^5.88)/g1^8 - 2*t^6. + 3*g1^4*t^6.06 + 3*g1^8*t^6.12 + g1^12*t^6.18 + g1^16*t^6.24 + (4*t^6.74)/g1 + 8*g1^3*t^6.79 + 6*g1^7*t^6.85 + 5*g1^11*t^6.91 + 3*g1^15*t^6.97 + t^7.35/g1^10 + t^7.41/g1^6 + (6*t^7.47)/g1^2 + 6*g1^2*t^7.53 + 6*g1^6*t^7.59 + 6*g1^10*t^7.65 + 3*g1^14*t^7.71 + 2*g1^18*t^7.77 + t^8.09/g1^11 + (3*t^8.15)/g1^7 - 5*g1*t^8.26 + 5*g1^9*t^8.38 + 5*g1^13*t^8.44 + 4*g1^17*t^8.5 + g1^21*t^8.56 + (5*t^8.82)/g1^12 - t^8.88/g1^8 - (6*t^8.94)/g1^4 - t^4.47/(g1^2*y) - t^6.68/(g1^5*y) - t^6.74/(g1*y) - t^7.41/(g1^6*y) + (2*t^7.47)/(g1^2*y) + (3*g1^2*t^7.53)/y + (2*g1^6*t^7.59)/y + (2*t^8.15)/(g1^7*y) + (6*t^8.21)/(g1^3*y) + (5*g1*t^8.26)/y + (2*g1^5*t^8.32)/y + (2*g1^9*t^8.38)/y + (g1^13*t^8.44)/y + t^8.94/(g1^4*y) - (t^4.47*y)/g1^2 - (t^6.68*y)/g1^5 - (t^6.74*y)/g1 - (t^7.41*y)/g1^6 + (2*t^7.47*y)/g1^2 + 3*g1^2*t^7.53*y + 2*g1^6*t^7.59*y + (2*t^8.15*y)/g1^7 + (6*t^8.21*y)/g1^3 + 5*g1*t^8.26*y + 2*g1^5*t^8.32*y + 2*g1^9*t^8.38*y + g1^13*t^8.44*y + (t^8.94*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 3222 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_3q_1\tilde{q}_1$ + $ M_3\phi_1q_2\tilde{q}_2$ + $ M_4\phi_1q_2\tilde{q}_1$ | 0.6318 | 0.8193 | 0.7712 | [X:[], M:[1.0, 0.8927, 0.7098, 0.7634], q:[0.7634, 0.2366], qb:[0.5268, 0.5805], phi:[0.4732]] | t^2.13 + 2*t^2.29 + t^2.45 + t^2.68 + 2*t^2.84 + t^3. + t^3.87 + t^4.03 + t^4.26 + 2*t^4.42 + 5*t^4.58 + 3*t^4.74 + t^4.81 + 2*t^4.9 + 3*t^4.97 + 5*t^5.13 + 4*t^5.29 + t^5.36 + t^5.45 + 2*t^5.52 + 4*t^5.68 - 2*t^6. - t^4.42/y - t^4.42*y | detail |