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 |
|---|---|---|---|---|---|---|---|---|---|
| 55491 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_1\tilde{q}_2$ + $ M_5\phi_1^2$ + $ M_2M_4$ + $ M_4M_6$ | 0.6043 | 0.7774 | 0.7773 | [X:[], M:[0.954, 1.138, 0.7989, 0.862, 0.954, 1.138], q:[0.7385, 0.3075], qb:[0.4626, 0.3995], phi:[0.523]] | [X:[], M:[[-4], [12], [26], [-12], [-4], [12]], q:[[-1], [5]], qb:[[-25], [13]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ M_3$, $ M_1$, $ M_5$, $ M_2$, $ M_6$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_3q_2\tilde{q}_2$, $ q_2^2\tilde{q}_1^2$, $ \phi_1q_1q_2$, $ M_3q_2\tilde{q}_1$, $ M_3^2$, $ \phi_1q_1\tilde{q}_2$, $ M_5q_2\tilde{q}_2$, $ \phi_1q_1\tilde{q}_1$, $ M_5q_2\tilde{q}_1$, $ M_1M_3$, $ M_3M_5$, $ M_6q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_1^2$, $ M_1M_5$, $ M_5^2$, $ M_6q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_2M_3$, $ M_3M_6$, $ M_3\phi_1q_2^2$, $ \phi_1q_2^2\tilde{q}_2^2$ | $\phi_1q_2^2\tilde{q}_1\tilde{q}_2$ | -2 | t^2.12 + t^2.31 + t^2.4 + 2*t^2.86 + 3*t^3.41 + t^3.69 + t^3.88 + t^3.97 + t^4.16 + t^4.24 + t^4.34 + t^4.43 + t^4.52 + t^4.62 + t^4.71 + t^4.79 + 2*t^4.98 + 2*t^5.17 + 2*t^5.26 + 2*t^5.53 + 4*t^5.72 + 3*t^5.81 - 2*t^6. + 2*t^6.09 + 5*t^6.28 + 2*t^6.36 + 2*t^6.55 + t^6.64 + t^6.65 + 2*t^6.74 + 6*t^6.83 + t^6.91 + t^6.93 + 4*t^7.1 + t^7.19 + t^7.21 + t^7.29 + 4*t^7.38 + t^7.48 + t^7.57 + 5*t^7.66 + t^7.76 + 2*t^7.84 + 3*t^7.93 + 3*t^8.03 + 2*t^8.12 + 4*t^8.21 + t^8.22 - 2*t^8.31 + 3*t^8.48 + t^8.5 + 3*t^8.59 + 4*t^8.67 + t^8.69 + 2*t^8.76 - 6*t^8.86 + 5*t^8.95 + t^8.96 - t^4.57/y - t^6.97/y + t^7.16/y + t^7.52/y + (2*t^7.71)/y + t^7.98/y + (3*t^8.17)/y + (2*t^8.26)/y + (3*t^8.53)/y + (4*t^8.72)/y + (4*t^8.81)/y - t^4.57*y - t^6.97*y + t^7.16*y + t^7.52*y + 2*t^7.71*y + t^7.98*y + 3*t^8.17*y + 2*t^8.26*y + 3*t^8.53*y + 4*t^8.72*y + 4*t^8.81*y | g1^18*t^2.12 + t^2.31/g1^20 + g1^26*t^2.4 + (2*t^2.86)/g1^4 + 3*g1^12*t^3.41 + g1^20*t^3.69 + t^3.88/g1^18 + g1^28*t^3.97 + t^4.16/g1^10 + g1^36*t^4.24 + t^4.34/g1^48 + t^4.43/g1^2 + g1^44*t^4.52 + t^4.62/g1^40 + g1^6*t^4.71 + g1^52*t^4.79 + 2*g1^14*t^4.98 + (2*t^5.17)/g1^24 + 2*g1^22*t^5.26 + 2*g1^30*t^5.53 + (4*t^5.72)/g1^8 + 3*g1^38*t^5.81 - 2*t^6. + 2*g1^46*t^6.09 + 5*g1^8*t^6.28 + 2*g1^54*t^6.36 + 2*g1^16*t^6.55 + g1^62*t^6.64 + t^6.65/g1^68 + (2*t^6.74)/g1^22 + 6*g1^24*t^6.83 + g1^70*t^6.91 + t^6.93/g1^60 + 4*g1^32*t^7.1 + g1^78*t^7.19 + t^7.21/g1^52 + t^7.29/g1^6 + 4*g1^40*t^7.38 + t^7.48/g1^44 + g1^2*t^7.57 + 5*g1^48*t^7.66 + t^7.76/g1^36 + 2*g1^10*t^7.84 + 3*g1^56*t^7.93 + (3*t^8.03)/g1^28 + 2*g1^18*t^8.12 + 4*g1^64*t^8.21 + t^8.22/g1^66 - (2*t^8.31)/g1^20 + 3*g1^72*t^8.48 + t^8.5/g1^58 + (3*t^8.59)/g1^12 + 4*g1^34*t^8.67 + t^8.69/g1^96 + 2*g1^80*t^8.76 - (6*t^8.86)/g1^4 + 5*g1^42*t^8.95 + t^8.96/g1^88 - (g1^2*t^4.57)/y - (g1^28*t^6.97)/y + t^7.16/(g1^10*y) + (g1^44*t^7.52)/y + (2*g1^6*t^7.71)/y + (g1^14*t^7.98)/y + (3*t^8.17)/(g1^24*y) + (2*g1^22*t^8.26)/y + (3*g1^30*t^8.53)/y + (4*t^8.72)/(g1^8*y) + (4*g1^38*t^8.81)/y - g1^2*t^4.57*y - g1^28*t^6.97*y + (t^7.16*y)/g1^10 + g1^44*t^7.52*y + 2*g1^6*t^7.71*y + g1^14*t^7.98*y + (3*t^8.17*y)/g1^24 + 2*g1^22*t^8.26*y + 3*g1^30*t^8.53*y + (4*t^8.72*y)/g1^8 + 4*g1^38*t^8.81*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47110 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_1\tilde{q}_2$ + $ M_5\phi_1^2$ + $ M_2M_4$ | 0.6167 | 0.7982 | 0.7726 | [X:[], M:[0.9519, 1.1442, 0.8125, 0.8558, 0.9519], q:[0.738, 0.3101], qb:[0.4495, 0.4063], phi:[0.524]] | t^2.15 + t^2.28 + t^2.44 + t^2.57 + 2*t^2.86 + 2*t^3.43 + t^3.72 + t^3.85 + t^4.01 + t^4.14 + t^4.27 + t^4.3 + t^4.43 + t^4.56 + t^4.59 + 2*t^4.72 + t^4.85 + t^4.88 + 3*t^5. + 3*t^5.13 + 2*t^5.29 + 2*t^5.42 + t^5.58 + 3*t^5.71 + 2*t^5.87 - t^4.57/y - t^4.57*y | detail |