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 |
|---|---|---|---|---|---|---|---|---|---|
| 46669 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_4\phi_1^2$ + $ M_4M_5$ | 0.7048 | 0.8625 | 0.8171 | [X:[], M:[1.0, 0.86, 1.0, 1.0467, 0.9533], q:[0.5233, 0.4767], qb:[0.6167, 0.4767], phi:[0.4767]] | [X:[], M:[[1, 1], [-6, 0], [-1, -1], [2, 0], [-2, 0]], q:[[1, 0], [-2, -1]], qb:[[5, 0], [0, 1]], phi:[[-1, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ M_5$, $ \phi_1^2$, $ M_3$, $ M_1$, $ q_2\tilde{q}_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_1q_2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1q_1^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_2^2$, $ M_2M_5$, $ M_2\phi_1^2$, $ M_5^2$, $ M_5\phi_1^2$, $ \phi_1^4$, $ M_3M_5$, $ M_3\phi_1^2$, $ M_2q_2\tilde{q}_1$, $ M_1M_5$, $ M_1\phi_1^2$, $ M_2\tilde{q}_1\tilde{q}_2$ | $M_1^2$, $ M_3^2$ | -3 | t^2.58 + 2*t^2.86 + 2*t^3. + 2*t^3.28 + 3*t^4.29 + 2*t^4.43 + t^4.57 + 2*t^4.71 + t^4.85 + t^5.13 + t^5.16 + 2*t^5.44 + 2*t^5.72 + 4*t^5.86 - 3*t^6. + 2*t^6.14 + 2*t^6.28 - 2*t^6.42 + 3*t^6.56 + 3*t^6.87 + 6*t^7.15 + 8*t^7.29 - 2*t^7.43 + 6*t^7.57 + 4*t^7.71 + t^7.74 - 2*t^7.85 + 4*t^7.99 + 2*t^8.02 + 2*t^8.13 - t^8.27 + 3*t^8.3 + 2*t^8.41 + 2*t^8.58 + 8*t^8.72 - 7*t^8.86 - t^4.43/y - t^7.01/y - t^7.29/y + t^7.57/y + t^7.85/y + (2*t^8.44)/y + (2*t^8.58)/y + t^8.72/y + (6*t^8.86)/y - t^4.43*y - t^7.01*y - t^7.29*y + t^7.57*y + t^7.85*y + 2*t^8.44*y + 2*t^8.58*y + t^8.72*y + 6*t^8.86*y | t^2.58/g1^6 + (2*t^2.86)/g1^2 + t^3./(g1*g2) + g1*g2*t^3. + (g1^3*t^3.28)/g2 + g1^5*g2*t^3.28 + t^4.29/g1^3 + t^4.29/(g1^5*g2^2) + (g2^2*t^4.29)/g1 + t^4.43/(g1^2*g2) + g2*t^4.43 + g1*t^4.57 + (g1^2*t^4.71)/g2 + g1^4*g2*t^4.71 + g1^5*t^4.85 + g1^9*t^5.13 + t^5.16/g1^12 + (2*t^5.44)/g1^8 + (2*t^5.72)/g1^4 + (2*t^5.86)/(g1^3*g2) + (2*g2*t^5.86)/g1 - 3*t^6. + (g1*t^6.14)/g2 + g1^3*g2*t^6.14 + (g1^2*t^6.28)/g2^2 + g1^6*g2^2*t^6.28 - (g1^5*t^6.42)/g2 - g1^7*g2*t^6.42 + g1^8*t^6.56 + (g1^6*t^6.56)/g2^2 + g1^10*g2^2*t^6.56 + t^6.87/g1^9 + t^6.87/(g1^11*g2^2) + (g2^2*t^6.87)/g1^7 + (2*t^7.15)/g1^5 + (2*t^7.15)/(g1^7*g2^2) + (2*g2^2*t^7.15)/g1^3 + t^7.29/(g1^6*g2^3) + (3*t^7.29)/(g1^4*g2) + (3*g2*t^7.29)/g1^2 + g2^3*t^7.29 - t^7.43/(g1^3*g2^2) - g1*g2^2*t^7.43 + t^7.57/(g1^2*g2^3) + (2*t^7.57)/g2 + 2*g1^2*g2*t^7.57 + g1^4*g2^3*t^7.57 + 2*g1^3*t^7.71 + (g1*t^7.71)/g2^2 + g1^5*g2^2*t^7.71 + t^7.74/g1^18 - (g1^4*t^7.85)/g2 - g1^6*g2*t^7.85 + 2*g1^7*t^7.99 + (g1^5*t^7.99)/g2^2 + g1^9*g2^2*t^7.99 + (2*t^8.02)/g1^14 + (g1^8*t^8.13)/g2 + g1^10*g2*t^8.13 - g1^11*t^8.27 + (3*t^8.3)/g1^10 + (g1^12*t^8.41)/g2 + g1^14*g2*t^8.41 + t^8.58/(g1^10*g2^4) + (g2^4*t^8.58)/g1^2 + t^8.72/(g1^7*g2^3) + (3*t^8.72)/(g1^5*g2) + (3*g2*t^8.72)/g1^3 + (g2^3*t^8.72)/g1 - (7*t^8.86)/g1^2 - t^4.43/(g1*y) - t^7.01/(g1^7*y) - t^7.29/(g1^3*y) + (g1*t^7.57)/y + (g1^5*t^7.85)/y + (2*t^8.44)/(g1^8*y) + t^8.58/(g1^7*g2*y) + (g2*t^8.58)/(g1^5*y) + t^8.72/(g1^4*y) + (3*t^8.86)/(g1^3*g2*y) + (3*g2*t^8.86)/(g1*y) - (t^4.43*y)/g1 - (t^7.01*y)/g1^7 - (t^7.29*y)/g1^3 + g1*t^7.57*y + g1^5*t^7.85*y + (2*t^8.44*y)/g1^8 + (t^8.58*y)/(g1^7*g2) + (g2*t^8.58*y)/g1^5 + (t^8.72*y)/g1^4 + (3*t^8.86*y)/(g1^3*g2) + (3*g2*t^8.86*y)/g1 |
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 |
|---|---|---|---|---|---|---|---|---|
| 46929 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_4\phi_1^2$ + $ M_4M_5$ + $ M_2q_2\tilde{q}_1$ | 0.7018 | 0.8592 | 0.8168 | [X:[], M:[0.9639, 0.8916, 1.0361, 1.0361, 0.9639], q:[0.5181, 0.5181], qb:[0.5903, 0.4458], phi:[0.4819]] | t^2.67 + 3*t^2.89 + 2*t^3.11 + t^3.33 + t^4.12 + 2*t^4.34 + 4*t^4.55 + 2*t^4.77 + t^4.99 + t^5.35 + 2*t^5.57 + 4*t^5.78 + t^6. - t^4.45/y - t^4.45*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46236 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_4\phi_1^2$ | 0.7008 | 0.8558 | 0.8188 | [X:[], M:[1.0, 0.8827, 1.0, 1.0391], q:[0.5195, 0.4805], qb:[0.5977, 0.4805], phi:[0.4805]] | t^2.65 + t^2.88 + 2*t^3. + t^3.12 + 2*t^3.23 + 3*t^4.32 + 2*t^4.44 + t^4.56 + 2*t^4.68 + t^4.79 + t^5.03 + t^5.3 + t^5.53 + t^5.77 + 2*t^5.88 - 2*t^6. - t^4.44/y - t^4.44*y | detail |