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 |
|---|---|---|---|---|---|---|---|---|---|
| 133 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_2^2$ | 0.6926 | 0.8437 | 0.8209 | [X:[], M:[0.6734, 1.0], q:[0.7908, 0.5357], qb:[0.5, 0.5], phi:[0.4184]] | [X:[], M:[[-8, 0], [0, 0]], q:[[1, 0], [7, 0]], qb:[[0, -1], [0, 1]], phi:[[-2, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ \phi_1^2$, $ M_2$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ q_1\tilde{q}_1$, $ q_1\tilde{q}_2$, $ M_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ M_1\phi_1^2$, $ M_1M_2$, $ \phi_1^4$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_2\phi_1^2$, $ \phi_1^2q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_2$ | . | -4 | t^2.02 + t^2.51 + t^3. + 2*t^3.11 + 2*t^3.87 + t^4.04 + 3*t^4.26 + 2*t^4.36 + t^4.47 + t^4.53 + 2*t^5.02 + 2*t^5.13 + t^5.51 + 2*t^5.62 - 4*t^6. + t^6.06 + 3*t^6.21 + 3*t^6.28 + 2*t^6.38 + t^6.55 + 2*t^6.77 + 2*t^6.87 + 4*t^6.98 + 2*t^7.04 - t^7.26 + 4*t^7.36 + 4*t^7.47 + 2*t^7.53 + 2*t^7.58 + 2*t^7.64 - 2*t^7.85 - t^7.96 - 3*t^8.02 + t^8.08 + 6*t^8.13 + 3*t^8.23 + 3*t^8.3 + t^8.51 + t^8.57 + 2*t^8.62 + 5*t^8.72 + 3*t^8.79 + 2*t^8.83 + 2*t^8.89 + t^8.94 - t^4.26/y - t^6.28/y - t^6.77/y + t^7.53/y + t^7.74/y + t^8.02/y + (2*t^8.13)/y + t^8.23/y - t^8.3/y + t^8.51/y + (2*t^8.62)/y - t^8.79/y + (2*t^8.89)/y - t^4.26*y - t^6.28*y - t^6.77*y + t^7.53*y + t^7.74*y + t^8.02*y + 2*t^8.13*y + t^8.23*y - t^8.3*y + t^8.51*y + 2*t^8.62*y - t^8.79*y + 2*t^8.89*y | t^2.02/g1^8 + t^2.51/g1^4 + t^3. + (g1^7*t^3.11)/g2 + g1^7*g2*t^3.11 + (g1*t^3.87)/g2 + g1*g2*t^3.87 + t^4.04/g1^16 + t^4.26/g1^2 + t^4.26/(g1^2*g2^2) + (g2^2*t^4.26)/g1^2 + (g1^5*t^4.36)/g2 + g1^5*g2*t^4.36 + g1^12*t^4.47 + t^4.53/g1^12 + (2*t^5.02)/g1^8 + t^5.13/(g1*g2) + (g2*t^5.13)/g1 + t^5.51/g1^4 + (g1^3*t^5.62)/g2 + g1^3*g2*t^5.62 - 2*t^6. - t^6./g2^2 - g2^2*t^6. + t^6.06/g1^24 + g1^14*t^6.21 + (g1^14*t^6.21)/g2^2 + g1^14*g2^2*t^6.21 + t^6.28/g1^10 + t^6.28/(g1^10*g2^2) + (g2^2*t^6.28)/g1^10 + t^6.38/(g1^3*g2) + (g2*t^6.38)/g1^3 + t^6.55/g1^20 + t^6.77/(g1^6*g2^2) + (g2^2*t^6.77)/g1^6 + (g1*t^6.87)/g2 + g1*g2*t^6.87 + 2*g1^8*t^6.98 + (g1^8*t^6.98)/g2^2 + g1^8*g2^2*t^6.98 + (2*t^7.04)/g1^16 - t^7.26/g1^2 + (g1^5*t^7.36)/g2^3 + (g1^5*t^7.36)/g2 + g1^5*g2*t^7.36 + g1^5*g2^3*t^7.36 + 2*g1^12*t^7.47 + (g1^12*t^7.47)/g2^2 + g1^12*g2^2*t^7.47 + (2*t^7.53)/g1^12 + (g1^19*t^7.58)/g2 + g1^19*g2*t^7.58 + t^7.64/(g1^5*g2) + (g2*t^7.64)/g1^5 - (g1^9*t^7.85)/g2 - g1^9*g2*t^7.85 - g1^16*t^7.96 - t^8.02/g1^8 - t^8.02/(g1^8*g2^2) - (g2^2*t^8.02)/g1^8 + t^8.08/g1^32 + t^8.13/(g1*g2^3) + (2*t^8.13)/(g1*g2) + (2*g2*t^8.13)/g1 + (g2^3*t^8.13)/g1 + g1^6*t^8.23 + (g1^6*t^8.23)/g2^2 + g1^6*g2^2*t^8.23 + t^8.3/g1^18 + t^8.3/(g1^18*g2^2) + (g2^2*t^8.3)/g1^18 - t^8.51/g1^4 + t^8.51/(g1^4*g2^4) + (g2^4*t^8.51)/g1^4 + t^8.57/g1^28 + (g1^3*t^8.62)/g2^3 + g1^3*g2^3*t^8.62 + g1^10*t^8.72 + (2*g1^10*t^8.72)/g2^2 + 2*g1^10*g2^2*t^8.72 + t^8.79/g1^14 + t^8.79/(g1^14*g2^2) + (g2^2*t^8.79)/g1^14 + (g1^17*t^8.83)/g2 + g1^17*g2*t^8.83 + t^8.89/(g1^7*g2) + (g2*t^8.89)/g1^7 + g1^24*t^8.94 - t^4.26/(g1^2*y) - t^6.28/(g1^10*y) - t^6.77/(g1^6*y) + t^7.53/(g1^12*y) + (g1^2*t^7.74)/y + t^8.02/(g1^8*y) + t^8.13/(g1*g2*y) + (g2*t^8.13)/(g1*y) + (g1^6*t^8.23)/y - t^8.3/(g1^18*y) + t^8.51/(g1^4*y) + (g1^3*t^8.62)/(g2*y) + (g1^3*g2*t^8.62)/y - t^8.79/(g1^14*y) + t^8.89/(g1^7*g2*y) + (g2*t^8.89)/(g1^7*y) - (t^4.26*y)/g1^2 - (t^6.28*y)/g1^10 - (t^6.77*y)/g1^6 + (t^7.53*y)/g1^12 + g1^2*t^7.74*y + (t^8.02*y)/g1^8 + (t^8.13*y)/(g1*g2) + (g2*t^8.13*y)/g1 + g1^6*t^8.23*y - (t^8.3*y)/g1^18 + (t^8.51*y)/g1^4 + (g1^3*t^8.62*y)/g2 + g1^3*g2*t^8.62*y - (t^8.79*y)/g1^14 + (t^8.89*y)/(g1^7*g2) + (g2*t^8.89*y)/g1^7 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 81 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ | 0.7025 | 0.8516 | 0.8249 | [X:[], M:[0.6751, 0.8682], q:[0.8071, 0.5178], qb:[0.5659, 0.5659], phi:[0.3858]] | t^2.03 + t^2.31 + t^2.6 + 2*t^3.25 + t^4.05 + 2*t^4.12 + t^4.26 + t^4.34 + 2*t^4.41 + 3*t^4.55 + 2*t^4.63 + t^4.92 + t^5.21 + 2*t^5.28 + 2*t^5.57 - 5*t^6. - t^4.16/y - t^4.16*y | detail |