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 |
|---|---|---|---|---|---|---|---|---|---|
| 2119 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2\tilde{q}_2$ + $ M_2M_5$ + $ M_6\phi_1q_2^2$ + $ M_6q_1\tilde{q}_2$ + $ M_7q_1\tilde{q}_2$ | 0.7176 | 0.9089 | 0.7895 | [X:[], M:[0.9983, 1.1256, 0.9363, 0.6884, 0.8744, 0.7504, 0.7504], q:[0.7814, 0.4062], qb:[0.5955, 0.4682], phi:[0.4372]] | [X:[], M:[[32], [-12], [22], [-18], [12], [-8], [-8]], q:[[-3], [1]], qb:[[-33], [11]], phi:[[6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_6$, $ M_7$, $ M_5$, $ \phi_1^2$, $ M_3$, $ M_1$, $ q_1q_2$, $ \phi_1\tilde{q}_2^2$, $ M_4^2$, $ q_1\tilde{q}_1$, $ M_4M_6$, $ M_4M_7$, $ \phi_1q_2\tilde{q}_1$, $ M_6^2$, $ M_6M_7$, $ M_7^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_4M_5$, $ M_4\phi_1^2$, $ M_3M_4$, $ M_5M_6$, $ M_5M_7$, $ M_6\phi_1^2$, $ M_7\phi_1^2$, $ \phi_1\tilde{q}_1^2$, $ M_1M_4$, $ M_3M_6$, $ M_3M_7$, $ M_5^2$, $ M_1M_6$, $ M_1M_7$, $ M_5\phi_1^2$, $ \phi_1^4$, $ M_3M_5$, $ M_3\phi_1^2$, $ M_3^2$, $ M_1M_5$, $ M_1\phi_1^2$, $ M_4q_1q_2$, $ M_1M_3$, $ M_6q_1q_2$, $ M_7q_1q_2$, $ M_1^2$ | . | -3 | t^2.07 + 2*t^2.25 + 2*t^2.62 + t^2.81 + t^2.99 + t^3.56 + t^4.12 + 2*t^4.13 + 3*t^4.32 + 4*t^4.5 + 2*t^4.69 + 5*t^4.87 + t^4.88 + 3*t^5.06 + 5*t^5.25 + t^5.43 + 2*t^5.62 + t^5.63 + t^5.8 + t^5.81 + t^5.99 - 3*t^6. + t^6.19 + 2*t^6.2 + 2*t^6.37 + 4*t^6.38 + 5*t^6.57 + t^6.74 + 8*t^6.75 + 6*t^6.94 + t^6.95 + t^7.12 + 10*t^7.13 + 2*t^7.14 + 7*t^7.31 + 8*t^7.5 + t^7.51 + 4*t^7.68 + t^7.69 + 8*t^7.87 + 4*t^8.06 - 3*t^8.07 + 5*t^8.24 - 7*t^8.25 + 2*t^8.26 + 2*t^8.43 - t^8.44 + 5*t^8.45 + 2*t^8.61 - 3*t^8.62 + 6*t^8.63 + t^8.8 - 3*t^8.81 + 8*t^8.82 + t^8.98 - 3*t^8.99 - t^4.31/y - t^6.38/y - (2*t^6.56)/y - t^6.93/y - t^7.12/y - t^7.31/y + (3*t^7.32)/y + (2*t^7.5)/y + (3*t^7.69)/y + (5*t^7.87)/y + (5*t^8.06)/y + (4*t^8.25)/y + (2*t^8.43)/y - t^8.44/y + (2*t^8.62)/y - t^8.63/y + t^8.8/y - t^8.81/y - t^4.31*y - t^6.38*y - 2*t^6.56*y - t^6.93*y - t^7.12*y - t^7.31*y + 3*t^7.32*y + 2*t^7.5*y + 3*t^7.69*y + 5*t^7.87*y + 5*t^8.06*y + 4*t^8.25*y + 2*t^8.43*y - t^8.44*y + 2*t^8.62*y - t^8.63*y + t^8.8*y - t^8.81*y | t^2.07/g1^18 + (2*t^2.25)/g1^8 + 2*g1^12*t^2.62 + g1^22*t^2.81 + g1^32*t^2.99 + t^3.56/g1^2 + g1^28*t^4.12 + (2*t^4.13)/g1^36 + (3*t^4.32)/g1^26 + (4*t^4.5)/g1^16 + (2*t^4.69)/g1^6 + 5*g1^4*t^4.87 + t^4.88/g1^60 + 3*g1^14*t^5.06 + 5*g1^24*t^5.25 + g1^34*t^5.43 + 2*g1^44*t^5.62 + t^5.63/g1^20 + g1^54*t^5.8 + t^5.81/g1^10 + g1^64*t^5.99 - 3*t^6. + g1^10*t^6.19 + (2*t^6.2)/g1^54 + 2*g1^20*t^6.37 + (4*t^6.38)/g1^44 + (5*t^6.57)/g1^34 + g1^40*t^6.74 + (8*t^6.75)/g1^24 + (6*t^6.94)/g1^14 + t^6.95/g1^78 + g1^60*t^7.12 + (10*t^7.13)/g1^4 + (2*t^7.14)/g1^68 + 7*g1^6*t^7.31 + 8*g1^16*t^7.5 + t^7.51/g1^48 + 4*g1^26*t^7.68 + t^7.69/g1^38 + 8*g1^36*t^7.87 + 4*g1^46*t^8.06 - (3*t^8.07)/g1^18 + 5*g1^56*t^8.24 - (7*t^8.25)/g1^8 + (2*t^8.26)/g1^72 + 2*g1^66*t^8.43 - g1^2*t^8.44 + (5*t^8.45)/g1^62 + 2*g1^76*t^8.61 - 3*g1^12*t^8.62 + (6*t^8.63)/g1^52 + g1^86*t^8.8 - 3*g1^22*t^8.81 + (8*t^8.82)/g1^42 + g1^96*t^8.98 - 3*g1^32*t^8.99 - (g1^6*t^4.31)/y - t^6.38/(g1^12*y) - (2*t^6.56)/(g1^2*y) - (g1^18*t^6.93)/y - (g1^28*t^7.12)/y - (g1^38*t^7.31)/y + (3*t^7.32)/(g1^26*y) + (2*t^7.5)/(g1^16*y) + (3*t^7.69)/(g1^6*y) + (5*g1^4*t^7.87)/y + (5*g1^14*t^8.06)/y + (4*g1^24*t^8.25)/y + (2*g1^34*t^8.43)/y - t^8.44/(g1^30*y) + (2*g1^44*t^8.62)/y - t^8.63/(g1^20*y) + (g1^54*t^8.8)/y - t^8.81/(g1^10*y) - g1^6*t^4.31*y - (t^6.38*y)/g1^12 - (2*t^6.56*y)/g1^2 - g1^18*t^6.93*y - g1^28*t^7.12*y - g1^38*t^7.31*y + (3*t^7.32*y)/g1^26 + (2*t^7.5*y)/g1^16 + (3*t^7.69*y)/g1^6 + 5*g1^4*t^7.87*y + 5*g1^14*t^8.06*y + 4*g1^24*t^8.25*y + 2*g1^34*t^8.43*y - (t^8.44*y)/g1^30 + 2*g1^44*t^8.62*y - (t^8.63*y)/g1^20 + g1^54*t^8.8*y - (t^8.81*y)/g1^10 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1060 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2\tilde{q}_2$ + $ M_2M_5$ + $ M_6\phi_1q_2^2$ + $ M_6q_1\tilde{q}_2$ | 0.6986 | 0.8743 | 0.799 | [X:[], M:[0.9932, 1.1276, 0.9328, 0.6913, 0.8724, 0.7517], q:[0.7819, 0.406], qb:[0.6008, 0.4664], phi:[0.4362]] | t^2.07 + t^2.26 + 2*t^2.62 + t^2.8 + t^2.98 + t^3.56 + t^3.74 + t^4.11 + 2*t^4.15 + 2*t^4.33 + 2*t^4.51 + 2*t^4.69 + 3*t^4.87 + t^4.91 + 2*t^5.05 + 4*t^5.23 + t^5.42 + 2*t^5.6 + t^5.64 + t^5.78 + t^5.82 + t^5.96 - 2*t^6. - t^4.31/y - t^4.31*y | detail |