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 |
|---|---|---|---|---|---|---|---|---|---|
| 46551 | SU2adj1nf2 | $\phi_1q_1q_2$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ \phi_1\tilde{q}_1\tilde{q}_2^3$ + $ M_3\phi_1\tilde{q}_2^2$ + $ M_4q_1\tilde{q}_1$ | 0.5734 | 0.743 | 0.7718 | [X:[], M:[0.8579, 1.1421, 0.7131, 0.7187], q:[0.9972, 0.5738], qb:[0.2841, 0.429], phi:[0.429]] | [X:[], M:[[2], [-2], [-3], [11]], q:[[-7], [6]], qb:[[-4], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ \tilde{q}_1\tilde{q}_2$, $ M_4$, $ M_1$, $ \phi_1^2$, $ \phi_1\tilde{q}_1^2$, $ q_2\tilde{q}_2$, $ M_2$, $ M_3^2$, $ q_1\tilde{q}_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_3M_4$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ M_1M_3$, $ M_3\phi_1^2$, $ q_1q_2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ M_1M_4$, $ M_4\phi_1^2$, $ M_3\phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1^3\tilde{q}_2$, $ M_1^2$, $ M_1\phi_1^2$, $ \phi_1^4$, $ M_4\phi_1\tilde{q}_1^2$, $ M_3q_2\tilde{q}_2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_4q_2\tilde{q}_2$, $ M_2M_3$, $ \phi_1^3\tilde{q}_1^2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ M_2M_4$, $ M_1q_2\tilde{q}_2$, $ \phi_1^2\tilde{q}_1^4$ | $M_1M_2$ | -1 | 2*t^2.14 + t^2.16 + 2*t^2.57 + t^2.99 + t^3.01 + t^3.43 + 4*t^4.28 + 2*t^4.3 + t^4.31 + 5*t^4.71 + 2*t^4.73 + 2*t^5.13 + 5*t^5.15 + t^5.16 + 3*t^5.57 + 2*t^5.58 + t^5.98 - t^6. + t^6.02 + 5*t^6.42 + 2*t^6.43 + 2*t^6.45 + t^6.47 + 6*t^6.85 + 4*t^6.87 + 2*t^6.89 + 3*t^7.27 + 8*t^7.29 + 5*t^7.3 + t^7.32 + 4*t^7.7 + 6*t^7.72 + 2*t^7.74 + 2*t^8.12 - 3*t^8.14 + t^8.16 + t^8.17 + 7*t^8.56 - 3*t^8.57 + 3*t^8.59 + 2*t^8.61 + t^8.62 + t^8.97 + 3*t^8.99 - t^4.29/y - t^6.43/y - t^6.44/y - t^6.86/y + t^7.28/y + (2*t^7.3)/y + (5*t^7.71)/y + (2*t^7.73)/y + (3*t^8.13)/y + (5*t^8.15)/y + t^8.16/y + (3*t^8.57)/y + (2*t^8.58)/y - t^8.6/y - t^4.29*y - t^6.43*y - t^6.44*y - t^6.86*y + t^7.28*y + 2*t^7.3*y + 5*t^7.71*y + 2*t^7.73*y + 3*t^8.13*y + 5*t^8.15*y + t^8.16*y + 3*t^8.57*y + 2*t^8.58*y - t^8.6*y | (2*t^2.14)/g1^3 + g1^11*t^2.16 + 2*g1^2*t^2.57 + t^2.99/g1^7 + g1^7*t^3.01 + t^3.43/g1^2 + (4*t^4.28)/g1^6 + 2*g1^8*t^4.3 + g1^22*t^4.31 + (5*t^4.71)/g1 + 2*g1^13*t^4.73 + (2*t^5.13)/g1^10 + 5*g1^4*t^5.15 + g1^18*t^5.16 + (3*t^5.57)/g1^5 + 2*g1^9*t^5.58 + t^5.98/g1^14 - t^6. + g1^14*t^6.02 + (5*t^6.42)/g1^9 + 2*g1^5*t^6.43 + 2*g1^19*t^6.45 + g1^33*t^6.47 + (6*t^6.85)/g1^4 + 4*g1^10*t^6.87 + 2*g1^24*t^6.89 + (3*t^7.27)/g1^13 + 8*g1*t^7.29 + 5*g1^15*t^7.3 + g1^29*t^7.32 + (4*t^7.7)/g1^8 + 6*g1^6*t^7.72 + 2*g1^20*t^7.74 + (2*t^8.12)/g1^17 - (3*t^8.14)/g1^3 + g1^11*t^8.16 + g1^25*t^8.17 + (7*t^8.56)/g1^12 - 3*g1^2*t^8.57 + 3*g1^16*t^8.59 + 2*g1^30*t^8.61 + g1^44*t^8.62 + t^8.97/g1^21 + (3*t^8.99)/g1^7 - (g1*t^4.29)/y - t^6.43/(g1^2*y) - (g1^12*t^6.44)/y - (g1^3*t^6.86)/y + t^7.28/(g1^6*y) + (2*g1^8*t^7.3)/y + (5*t^7.71)/(g1*y) + (2*g1^13*t^7.73)/y + (3*t^8.13)/(g1^10*y) + (5*g1^4*t^8.15)/y + (g1^18*t^8.16)/y + (3*t^8.57)/(g1^5*y) + (2*g1^9*t^8.58)/y - (g1^23*t^8.6)/y - g1*t^4.29*y - (t^6.43*y)/g1^2 - g1^12*t^6.44*y - g1^3*t^6.86*y + (t^7.28*y)/g1^6 + 2*g1^8*t^7.3*y + (5*t^7.71*y)/g1 + 2*g1^13*t^7.73*y + (3*t^8.13*y)/g1^10 + 5*g1^4*t^8.15*y + g1^18*t^8.16*y + (3*t^8.57*y)/g1^5 + 2*g1^9*t^8.58*y - g1^23*t^8.6*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 |
|---|---|---|---|---|---|---|---|---|
| 47178 | $\phi_1q_1q_2$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ \phi_1\tilde{q}_1\tilde{q}_2^3$ + $ M_3\phi_1\tilde{q}_2^2$ + $ M_4q_1\tilde{q}_1$ + $ M_5\phi_1\tilde{q}_1^2$ | 0.5745 | 0.7465 | 0.7697 | [X:[], M:[0.8498, 1.1502, 0.7253, 0.674, 0.9744], q:[1.0256, 0.5495], qb:[0.3004, 0.4249], phi:[0.4249]] | t^2.02 + 2*t^2.18 + 2*t^2.55 + 2*t^2.92 + t^3.45 + t^4.04 + 2*t^4.2 + 4*t^4.35 + 2*t^4.57 + 5*t^4.73 + 2*t^4.95 + 6*t^5.1 + 4*t^5.47 + t^5.63 + 3*t^5.85 - 2*t^6. - t^4.27/y - t^4.27*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46330 | SU2adj1nf2 | $\phi_1q_1q_2$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ \phi_1\tilde{q}_1\tilde{q}_2^3$ + $ M_3\phi_1\tilde{q}_2^2$ | 0.5538 | 0.7072 | 0.783 | [X:[], M:[0.8638, 1.1362, 0.7043], q:[0.9766, 0.5914], qb:[0.2724, 0.4319], phi:[0.4319]] | 2*t^2.11 + 2*t^2.59 + t^2.93 + t^3.07 + t^3.41 + t^3.75 + 4*t^4.23 + 5*t^4.7 + 2*t^5.04 + 4*t^5.18 + 3*t^5.52 + t^5.66 + 3*t^5.86 - t^6. - t^4.3/y - t^4.3*y | detail |