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 |
|---|---|---|---|---|---|---|---|---|---|
| 5148 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_4\phi_1q_2^2$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1\tilde{q}_1$ + $ M_5q_1\tilde{q}_2$ + $ M_5M_7$ + $ M_3M_8$ | 0.6051 | 0.7779 | 0.7779 | [X:[], M:[1.0, 0.9947, 1.0106, 0.9947, 0.754, 0.7593, 1.246, 0.9894], q:[0.7487, 0.2513], qb:[0.4921, 0.4974], phi:[0.5026]] | [X:[], M:[[0], [4], [-8], [4], [-3], [-7], [3], [8]], q:[[1], [-1]], qb:[[6], [2]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ M_6$, $ M_8$, $ M_2$, $ M_4$, $ M_1$, $ M_7$, $ q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ \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$, $ \phi_1q_1q_2$, $ M_6q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_2$, $ M_6^2$, $ M_8q_2\tilde{q}_1$, $ M_2q_2\tilde{q}_1$, $ M_4q_2\tilde{q}_1$, $ M_8q_2\tilde{q}_2$, $ \phi_1q_1\tilde{q}_1$, $ M_2q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_2$, $ M_6M_8$, $ \phi_1q_1\tilde{q}_2$, $ M_2M_6$, $ M_4M_6$, $ M_8^2$, $ M_2M_8$, $ M_4M_8$, $ M_2^2$, $ M_2M_4$, $ M_4^2$, $ M_1M_8$, $ M_7q_2\tilde{q}_1$, $ M_1M_2$, $ M_1M_4$, $ M_7q_2\tilde{q}_2$, $ q_1q_2\tilde{q}_2^2$ | $\phi_1q_2^2\tilde{q}_2^2$ | -2 | t^2.23 + t^2.25 + t^2.28 + t^2.97 + 2*t^2.98 + t^3. + 2*t^3.74 + t^3.75 + 2*t^4.46 + 2*t^4.48 + 2*t^4.49 + t^4.51 + t^4.52 + t^4.56 + t^5.2 + 3*t^5.21 + 3*t^5.23 + 2*t^5.25 + t^5.26 + t^5.94 + 2*t^5.95 + 5*t^5.97 + 3*t^5.98 - 2*t^6. + t^6.03 + 2*t^6.69 + 4*t^6.71 + 5*t^6.72 + 4*t^6.74 + t^6.8 + t^6.83 + 2*t^7.43 + 5*t^7.44 + 6*t^7.46 + 6*t^7.48 + t^7.49 - t^7.51 + t^7.54 + t^8.17 + 3*t^8.18 + 8*t^8.2 + 7*t^8.21 + t^8.23 - 2*t^8.25 - 2*t^8.26 - 3*t^8.28 + t^8.31 + t^8.9 + 5*t^8.92 + 8*t^8.94 + 10*t^8.95 + 4*t^8.97 - 3*t^8.98 - t^4.51/y - t^6.79/y + t^7.48/y - t^7.49/y + t^7.51/y + (2*t^7.52)/y + t^8.2/y + (3*t^8.21)/y + (4*t^8.23)/y + (2*t^8.25)/y + (2*t^8.26)/y + t^8.28/y + (2*t^8.95)/y + (4*t^8.97)/y + (5*t^8.98)/y - t^4.51*y - t^6.79*y + t^7.48*y - t^7.49*y + t^7.51*y + 2*t^7.52*y + t^8.2*y + 3*t^8.21*y + 4*t^8.23*y + 2*t^8.25*y + 2*t^8.26*y + t^8.28*y + 2*t^8.95*y + 4*t^8.97*y + 5*t^8.98*y | g1^5*t^2.23 + g1*t^2.25 + t^2.28/g1^7 + g1^8*t^2.97 + 2*g1^4*t^2.98 + t^3. + 2*g1^3*t^3.74 + t^3.75/g1 + 2*g1^10*t^4.46 + 2*g1^6*t^4.48 + 2*g1^2*t^4.49 + t^4.51/g1^2 + t^4.52/g1^6 + t^4.56/g1^14 + g1^13*t^5.2 + 3*g1^9*t^5.21 + 3*g1^5*t^5.23 + 2*g1*t^5.25 + t^5.26/g1^3 + g1^16*t^5.94 + 2*g1^12*t^5.95 + 5*g1^8*t^5.97 + 3*g1^4*t^5.98 - 2*t^6. + t^6.03/g1^8 + 2*g1^15*t^6.69 + 4*g1^11*t^6.71 + 5*g1^7*t^6.72 + 4*g1^3*t^6.74 + t^6.8/g1^13 + t^6.83/g1^21 + 2*g1^18*t^7.43 + 5*g1^14*t^7.44 + 6*g1^10*t^7.46 + 6*g1^6*t^7.48 + g1^2*t^7.49 - t^7.51/g1^2 + t^7.54/g1^10 + g1^21*t^8.17 + 3*g1^17*t^8.18 + 8*g1^13*t^8.2 + 7*g1^9*t^8.21 + g1^5*t^8.23 - 2*g1*t^8.25 - (2*t^8.26)/g1^3 - (3*t^8.28)/g1^7 + t^8.31/g1^15 + g1^24*t^8.9 + 5*g1^20*t^8.92 + 8*g1^16*t^8.94 + 10*g1^12*t^8.95 + 4*g1^8*t^8.97 - 3*g1^4*t^8.98 - t^4.51/(g1^2*y) - t^6.79/(g1^9*y) + (g1^6*t^7.48)/y - (g1^2*t^7.49)/y + t^7.51/(g1^2*y) + (2*t^7.52)/(g1^6*y) + (g1^13*t^8.2)/y + (3*g1^9*t^8.21)/y + (4*g1^5*t^8.23)/y + (2*g1*t^8.25)/y + (2*t^8.26)/(g1^3*y) + t^8.28/(g1^7*y) + (2*g1^12*t^8.95)/y + (4*g1^8*t^8.97)/y + (5*g1^4*t^8.98)/y - (t^4.51*y)/g1^2 - (t^6.79*y)/g1^9 + g1^6*t^7.48*y - g1^2*t^7.49*y + (t^7.51*y)/g1^2 + (2*t^7.52*y)/g1^6 + g1^13*t^8.2*y + 3*g1^9*t^8.21*y + 4*g1^5*t^8.23*y + 2*g1*t^8.25*y + (2*t^8.26*y)/g1^3 + (t^8.28*y)/g1^7 + 2*g1^12*t^8.95*y + 4*g1^8*t^8.97*y + 5*g1^4*t^8.98*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 |
|---|---|---|---|---|---|---|---|---|---|
| 3467 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_4\phi_1q_2^2$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1\tilde{q}_1$ + $ M_5q_1\tilde{q}_2$ + $ M_5M_7$ | 0.6068 | 0.7776 | 0.7804 | [X:[], M:[1.0, 1.0238, 0.9523, 1.0238, 0.7321, 0.7083, 1.2679], q:[0.756, 0.244], qb:[0.5358, 0.5119], phi:[0.4881]] | t^2.12 + t^2.27 + t^2.34 + t^2.86 + t^3. + 2*t^3.07 + t^3.73 + 2*t^3.8 + t^4.25 + t^4.39 + t^4.46 + 2*t^4.54 + 2*t^4.61 + 2*t^4.68 + t^4.98 + t^5.12 + 2*t^5.2 + t^5.27 + 3*t^5.34 + 2*t^5.41 + t^5.71 + 2*t^5.86 + 2*t^5.93 - 2*t^6. - t^4.46/y - t^4.46*y | detail |