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 |
|---|---|---|---|---|---|---|---|---|---|
| 55331 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3\phi_1q_2^2$ + $ M_1M_4$ + $ M_3M_5$ + $ M_6\tilde{q}_1\tilde{q}_2$ | 0.5958 | 0.764 | 0.7799 | [X:[], M:[0.9557, 0.7879, 0.8671, 1.0443, 1.1329, 1.1329], q:[0.7389, 0.3054], qb:[0.4732, 0.394], phi:[0.5221]] | [X:[], M:[[-4], [26], [-12], [4], [12], [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_2$, $ M_4$, $ \phi_1^2$, $ M_5$, $ 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_2q_2\tilde{q}_2$, $ q_2^2\tilde{q}_1^2$, $ \phi_1q_1q_2$, $ M_2q_2\tilde{q}_1$, $ M_2^2$, $ M_4q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_2M_4$, $ M_2\phi_1^2$, $ M_5q_2\tilde{q}_2$, $ M_6q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_5q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_2M_5$, $ M_2M_6$, $ M_2\phi_1q_2^2$, $ \phi_1q_2^2\tilde{q}_2^2$ | $\phi_1q_2^2\tilde{q}_1\tilde{q}_2$ | -2 | t^2.1 + t^2.34 + t^2.36 + 2*t^3.13 + 3*t^3.4 + t^3.66 + t^3.9 + t^3.93 + t^4.17 + t^4.2 + t^4.41 + t^4.43 + t^4.46 + t^4.67 + t^4.7 + t^4.73 + 2*t^5.23 + 2*t^5.47 + 4*t^5.5 + t^5.73 + 3*t^5.76 - 2*t^6. + 2*t^6.03 + 2*t^6.27 + 2*t^6.29 + 6*t^6.53 + t^6.56 + t^6.74 + 6*t^6.8 + t^6.83 + t^7.01 + 4*t^7.06 + t^7.09 - t^7.27 + t^7.3 + 4*t^7.33 + t^7.54 + t^7.57 + 5*t^7.59 + 3*t^7.8 + t^7.83 + 5*t^7.86 - t^8.1 + 4*t^8.13 + t^8.31 - 2*t^8.34 - t^8.36 + 3*t^8.39 + t^8.57 + 5*t^8.63 + 2*t^8.66 + t^8.81 + 7*t^8.9 + t^8.92 - t^4.57/y - t^6.93/y + t^7.17/y + (2*t^7.43)/y + t^7.46/y - t^7.97/y + t^8.2/y + (2*t^8.23)/y + (2*t^8.47)/y + (5*t^8.5)/y + (3*t^8.73)/y + (4*t^8.76)/y - t^4.57*y - t^6.93*y + t^7.17*y + 2*t^7.43*y + t^7.46*y - t^7.97*y + t^8.2*y + 2*t^8.23*y + 2*t^8.47*y + 5*t^8.5*y + 3*t^8.73*y + 4*t^8.76*y | g1^18*t^2.1 + t^2.34/g1^20 + g1^26*t^2.36 + 2*g1^4*t^3.13 + 3*g1^12*t^3.4 + g1^20*t^3.66 + t^3.9/g1^18 + g1^28*t^3.93 + t^4.17/g1^10 + g1^36*t^4.2 + t^4.41/g1^48 + t^4.43/g1^2 + g1^44*t^4.46 + t^4.67/g1^40 + g1^6*t^4.7 + g1^52*t^4.73 + 2*g1^22*t^5.23 + (2*t^5.47)/g1^16 + 4*g1^30*t^5.5 + t^5.73/g1^8 + 3*g1^38*t^5.76 - 2*t^6. + 2*g1^46*t^6.03 + 2*g1^8*t^6.27 + 2*g1^54*t^6.29 + 6*g1^16*t^6.53 + g1^62*t^6.56 + t^6.74/g1^68 + 6*g1^24*t^6.8 + g1^70*t^6.83 + t^7.01/g1^60 + 4*g1^32*t^7.06 + g1^78*t^7.09 - t^7.27/g1^52 + t^7.3/g1^6 + 4*g1^40*t^7.33 + t^7.54/g1^44 + g1^2*t^7.57 + 5*g1^48*t^7.59 + (3*t^7.8)/g1^36 + g1^10*t^7.83 + 5*g1^56*t^7.86 - g1^18*t^8.1 + 4*g1^64*t^8.13 + t^8.31/g1^66 - (2*t^8.34)/g1^20 - g1^26*t^8.36 + 3*g1^72*t^8.39 + t^8.57/g1^58 + 5*g1^34*t^8.63 + 2*g1^80*t^8.66 + t^8.81/g1^96 + 7*g1^42*t^8.9 + g1^88*t^8.92 - (g1^2*t^4.57)/y - (g1^28*t^6.93)/y + t^7.17/(g1^10*y) + (2*t^7.43)/(g1^2*y) + (g1^44*t^7.46)/y - (g1^14*t^7.97)/y + t^8.2/(g1^24*y) + (2*g1^22*t^8.23)/y + (2*t^8.47)/(g1^16*y) + (5*g1^30*t^8.5)/y + (3*t^8.73)/(g1^8*y) + (4*g1^38*t^8.76)/y - g1^2*t^4.57*y - g1^28*t^6.93*y + (t^7.17*y)/g1^10 + (2*t^7.43*y)/g1^2 + g1^44*t^7.46*y - g1^14*t^7.97*y + (t^8.2*y)/g1^24 + 2*g1^22*t^8.23*y + (2*t^8.47*y)/g1^16 + 5*g1^30*t^8.5*y + (3*t^8.73*y)/g1^8 + 4*g1^38*t^8.76*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47064 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3\phi_1q_2^2$ + $ M_1M_4$ + $ M_3M_5$ | 0.6079 | 0.7838 | 0.7756 | [X:[], M:[0.9536, 0.8018, 0.8607, 1.0464, 1.1393], q:[0.7384, 0.308], qb:[0.4598, 0.4009], phi:[0.5232]] | t^2.13 + t^2.3 + t^2.41 + t^2.58 + 2*t^3.14 + 2*t^3.42 + t^3.7 + t^3.87 + t^3.98 + t^4.15 + t^4.25 + t^4.33 + t^4.43 + t^4.53 + t^4.61 + 2*t^4.71 + t^4.81 + t^4.89 + t^4.99 + t^5.16 + 2*t^5.27 + 2*t^5.44 + 3*t^5.54 + 2*t^5.72 + 2*t^5.82 - t^4.57/y - t^4.57*y | detail |