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 |
|---|---|---|---|---|---|---|---|---|---|
| 55357 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_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}_2$ + $ M_2M_5$ + $ M_6\phi_1^2$ | 0.6242 | 0.8106 | 0.7701 | [X:[], M:[1.0, 0.9818, 0.7432, 0.7432, 1.0182, 1.0091], q:[0.7523, 0.2477], qb:[0.5045, 0.5136], phi:[0.4955]] | [X:[], M:[[0], [-8], [-3], [-3], [8], [4]], 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_1q_2^2$, $ M_1$, $ M_6$, $ M_5$, $ \phi_1q_2\tilde{q}_1$, $ q_1\tilde{q}_2$, $ M_3^2$, $ M_3M_4$, $ M_4^2$, $ \phi_1q_1q_2$, $ M_3q_2\tilde{q}_1$, $ 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_1q_2^2$, $ M_4\phi_1q_2^2$, $ M_1M_3$, $ M_1M_4$, $ \phi_1q_2^3\tilde{q}_1$, $ M_3M_6$, $ M_4M_6$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_2$, $ M_3M_5$, $ M_4M_5$, $ M_6q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_5q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_2$, $ M_5q_2\tilde{q}_2$, $ \phi_1^2q_2^4$, $ M_3\phi_1q_2\tilde{q}_1$, $ M_4\phi_1q_2\tilde{q}_1$ | $M_6\phi_1q_2^2$, $ \phi_1q_2^2\tilde{q}_1^2$ | -1 | 2*t^2.23 + t^2.26 + t^2.28 + t^2.97 + t^3. + t^3.03 + t^3.05 + t^3.74 + t^3.8 + 3*t^4.46 + 2*t^4.49 + 4*t^4.51 + 2*t^4.54 + 2*t^4.57 + t^5.2 + 2*t^5.23 + 4*t^5.26 + 4*t^5.28 + 2*t^5.31 + t^5.34 + t^5.95 + t^5.97 - t^6. + 3*t^6.03 + 2*t^6.05 + 2*t^6.08 + t^6.11 + 3*t^6.69 + 2*t^6.72 + 5*t^6.74 + 4*t^6.77 + 6*t^6.8 + 3*t^6.82 + 3*t^6.85 + t^7.43 + t^7.46 + 5*t^7.49 + 5*t^7.51 + 7*t^7.54 + 6*t^7.57 + 4*t^7.6 + 2*t^7.62 + t^8.18 - 4*t^8.23 + t^8.26 + 6*t^8.31 + 5*t^8.34 + 4*t^8.37 + t^8.39 + 5*t^8.92 + t^8.95 + 3*t^8.97 - t^4.49/y - (2*t^6.72)/y + t^7.46/y + (2*t^7.49)/y + (2*t^7.51)/y + t^7.54/y + (2*t^8.2)/y + (3*t^8.23)/y + (6*t^8.26)/y + (4*t^8.28)/y + (2*t^8.31)/y + t^8.34/y - (3*t^8.95)/y + (3*t^8.97)/y - t^4.49*y - 2*t^6.72*y + t^7.46*y + 2*t^7.49*y + 2*t^7.51*y + t^7.54*y + 2*t^8.2*y + 3*t^8.23*y + 6*t^8.26*y + 4*t^8.28*y + 2*t^8.31*y + t^8.34*y - 3*t^8.95*y + 3*t^8.97*y | (2*t^2.23)/g1^3 + g1*t^2.26 + g1^5*t^2.28 + t^2.97/g1^4 + t^3. + g1^4*t^3.03 + g1^8*t^3.05 + t^3.74/g1 + g1^7*t^3.8 + (3*t^4.46)/g1^6 + (2*t^4.49)/g1^2 + 4*g1^2*t^4.51 + 2*g1^6*t^4.54 + 2*g1^10*t^4.57 + t^5.2/g1^7 + (2*t^5.23)/g1^3 + 4*g1*t^5.26 + 4*g1^5*t^5.28 + 2*g1^9*t^5.31 + g1^13*t^5.34 + t^5.95/g1^8 + t^5.97/g1^4 - t^6. + 3*g1^4*t^6.03 + 2*g1^8*t^6.05 + 2*g1^12*t^6.08 + g1^16*t^6.11 + (3*t^6.69)/g1^9 + (2*t^6.72)/g1^5 + (5*t^6.74)/g1 + 4*g1^3*t^6.77 + 6*g1^7*t^6.8 + 3*g1^11*t^6.82 + 3*g1^15*t^6.85 + t^7.43/g1^10 + t^7.46/g1^6 + (5*t^7.49)/g1^2 + 5*g1^2*t^7.51 + 7*g1^6*t^7.54 + 6*g1^10*t^7.57 + 4*g1^14*t^7.6 + 2*g1^18*t^7.62 + t^8.18/g1^11 - (4*t^8.23)/g1^3 + g1*t^8.26 + 6*g1^9*t^8.31 + 5*g1^13*t^8.34 + 4*g1^17*t^8.37 + g1^21*t^8.39 + (5*t^8.92)/g1^12 + t^8.95/g1^8 + (3*t^8.97)/g1^4 - t^4.49/(g1^2*y) - (2*t^6.72)/(g1^5*y) + t^7.46/(g1^6*y) + (2*t^7.49)/(g1^2*y) + (2*g1^2*t^7.51)/y + (g1^6*t^7.54)/y + (2*t^8.2)/(g1^7*y) + (3*t^8.23)/(g1^3*y) + (6*g1*t^8.26)/y + (4*g1^5*t^8.28)/y + (2*g1^9*t^8.31)/y + (g1^13*t^8.34)/y - (3*t^8.95)/(g1^8*y) + (3*t^8.97)/(g1^4*y) - (t^4.49*y)/g1^2 - (2*t^6.72*y)/g1^5 + (t^7.46*y)/g1^6 + (2*t^7.49*y)/g1^2 + 2*g1^2*t^7.51*y + g1^6*t^7.54*y + (2*t^8.2*y)/g1^7 + (3*t^8.23*y)/g1^3 + 6*g1*t^8.26*y + 4*g1^5*t^8.28*y + 2*g1^9*t^8.31*y + g1^13*t^8.34*y - (3*t^8.95*y)/g1^8 + (3*t^8.97*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46907 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_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}_2$ + $ M_2M_5$ | 0.6259 | 0.8118 | 0.7711 | [X:[], M:[1.0, 0.9469, 0.7301, 0.7301, 1.0531], q:[0.7566, 0.2434], qb:[0.5133, 0.5398], phi:[0.4867]] | 2*t^2.19 + t^2.27 + t^2.35 + 2*t^2.92 + t^3. + t^3.16 + t^3.73 + t^3.89 + 3*t^4.38 + 2*t^4.46 + 4*t^4.54 + 2*t^4.62 + 2*t^4.7 + 3*t^5.11 + 3*t^5.19 + 3*t^5.27 + 3*t^5.35 + t^5.43 + t^5.51 + 3*t^5.84 + 2*t^5.92 - 2*t^6. - t^4.46/y - t^4.46*y | detail |