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 |
|---|---|---|---|---|---|---|---|---|---|
| 48234 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ \phi_1q_2^2\tilde{q}_2^2$ + $ M_1M_3$ + $ M_4\phi_1q_2^2$ + $ M_5\phi_1q_2\tilde{q}_2$ | 0.6394 | 0.8382 | 0.7628 | [X:[], M:[0.9549, 0.829, 1.0451, 0.8646, 0.7387], q:[0.7387, 0.3064], qb:[0.4323, 0.4323], phi:[0.5226]] | [X:[], M:[[4], [-7], [-4], [12], [1]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ M_2$, $ M_4$, $ \tilde{q}_1\tilde{q}_2$, $ M_3$, $ \phi_1^2$, $ q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_5^2$, $ M_5q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_5q_2\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_2M_5$, $ \phi_1q_1q_2$, $ M_2q_2\tilde{q}_1$, $ M_2q_2\tilde{q}_2$, $ M_4M_5$, $ M_4q_2\tilde{q}_1$, $ M_4q_2\tilde{q}_2$, $ M_5\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_2^2$, $ M_2M_4$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_3M_5$, $ M_5\phi_1^2$, $ M_3q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_3M_4$, $ M_4\phi_1^2$, $ M_5q_1\tilde{q}_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ q_1q_2\tilde{q}_2^2$ | $M_5\phi_1q_2\tilde{q}_1$, $ \phi_1q_2^2\tilde{q}_1^2$ | 3*t^2.22 + t^2.49 + 2*t^2.59 + 2*t^3.14 + t^3.51 + t^3.78 + 3*t^4.16 + 6*t^4.43 + 3*t^4.7 + 6*t^4.81 + t^4.97 + 2*t^5.08 + 3*t^5.19 + 6*t^5.35 + 6*t^5.73 - 2*t^6. + 2*t^6.11 + 2*t^6.27 + 7*t^6.38 + 11*t^6.65 + 6*t^6.76 + 4*t^6.92 + 10*t^7.03 + t^7.19 + 8*t^7.3 + 9*t^7.4 + t^7.46 + 7*t^7.57 + 4*t^7.67 + 4*t^7.78 + 12*t^7.95 - 10*t^8.22 + 15*t^8.32 + t^8.49 + 2*t^8.59 + 3*t^8.7 - 2*t^8.76 + 17*t^8.86 + 13*t^8.97 - t^4.57/y - t^6.78/y - t^7.05/y - t^7.16/y + (4*t^7.43)/y + (2*t^7.7)/y + (6*t^7.81)/y + t^7.97/y + (3*t^8.08)/y + t^8.19/y + (7*t^8.35)/y + (2*t^8.62)/y + (7*t^8.73)/y - t^4.57*y - t^6.78*y - t^7.05*y - t^7.16*y + 4*t^7.43*y + 2*t^7.7*y + 6*t^7.81*y + t^7.97*y + 3*t^8.08*y + t^8.19*y + 7*t^8.35*y + 2*t^8.62*y + 7*t^8.73*y | 3*g1*t^2.22 + t^2.49/g1^7 + 2*g1^12*t^2.59 + (2*t^3.14)/g1^4 + g1^7*t^3.51 + t^3.78/g1 + 3*g1^10*t^4.16 + 6*g1^2*t^4.43 + (3*t^4.7)/g1^6 + 6*g1^13*t^4.81 + t^4.97/g1^14 + 2*g1^5*t^5.08 + 3*g1^24*t^5.19 + (6*t^5.35)/g1^3 + 6*g1^8*t^5.73 - 2*t^6. + 2*g1^19*t^6.11 + (2*t^6.27)/g1^8 + 7*g1^11*t^6.38 + 11*g1^3*t^6.65 + 6*g1^22*t^6.76 + (4*t^6.92)/g1^5 + 10*g1^14*t^7.03 + t^7.19/g1^13 + 8*g1^6*t^7.3 + 9*g1^25*t^7.4 + t^7.46/g1^21 + (7*t^7.57)/g1^2 + 4*g1^17*t^7.67 + 4*g1^36*t^7.78 + 12*g1^9*t^7.95 - 10*g1*t^8.22 + 15*g1^20*t^8.32 + t^8.49/g1^7 + 2*g1^12*t^8.59 + 3*g1^31*t^8.7 - (2*t^8.76)/g1^15 + 17*g1^4*t^8.86 + 13*g1^23*t^8.97 - t^4.57/(g1^2*y) - t^6.78/(g1*y) - t^7.05/(g1^9*y) - (g1^10*t^7.16)/y + (4*g1^2*t^7.43)/y + (2*t^7.7)/(g1^6*y) + (6*g1^13*t^7.81)/y + t^7.97/(g1^14*y) + (3*g1^5*t^8.08)/y + (g1^24*t^8.19)/y + (7*t^8.35)/(g1^3*y) + (2*t^8.62)/(g1^11*y) + (7*g1^8*t^8.73)/y - (t^4.57*y)/g1^2 - (t^6.78*y)/g1 - (t^7.05*y)/g1^9 - g1^10*t^7.16*y + 4*g1^2*t^7.43*y + (2*t^7.7*y)/g1^6 + 6*g1^13*t^7.81*y + (t^7.97*y)/g1^14 + 3*g1^5*t^8.08*y + g1^24*t^8.19*y + (7*t^8.35*y)/g1^3 + (2*t^8.62*y)/g1^11 + 7*g1^8*t^8.73*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46789 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ \phi_1q_2^2\tilde{q}_2^2$ + $ M_1M_3$ + $ M_4\phi_1q_2^2$ | 0.62 | 0.8023 | 0.7727 | [X:[], M:[0.9554, 0.828, 1.0446, 0.8663], q:[0.7389, 0.3057], qb:[0.4331, 0.4331], phi:[0.5223]] | 2*t^2.22 + t^2.48 + 2*t^2.6 + 2*t^3.13 + t^3.52 + 2*t^3.78 + 3*t^4.17 + 3*t^4.43 + 2*t^4.7 + 4*t^4.82 + t^4.97 + 2*t^5.08 + 3*t^5.2 + 4*t^5.35 + 5*t^5.73 - t^6. - t^4.57/y - t^4.57*y | detail |