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 |
|---|---|---|---|---|---|---|---|---|---|
| 2905 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ q_1q_2\tilde{q}_2^2$ + $ M_6q_1\tilde{q}_2$ | 0.6338 | 0.8277 | 0.7658 | [X:[], M:[0.9662, 1.1014, 0.9662, 0.8986, 0.7754, 0.7754], q:[0.7415, 0.2923], qb:[0.4155, 0.4831], phi:[0.5169]] | [X:[], M:[[4], [-12], [4], [12], [-3], [-3]], q:[[1], [-5]], qb:[[10], [2]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_2\tilde{q}_1$, $ M_5$, $ M_6$, $ q_2\tilde{q}_2$, $ M_4$, $ M_1$, $ M_3$, $ \phi_1q_2^2$, $ q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_5q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_5^2$, $ M_5M_6$, $ M_6^2$, $ \phi_1q_1q_2$, $ M_5q_2\tilde{q}_2$, $ M_6q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_4q_2\tilde{q}_1$, $ M_4M_5$, $ M_4M_6$, $ \phi_1q_1\tilde{q}_1$, $ M_3q_2\tilde{q}_1$, $ M_4q_2\tilde{q}_2$, $ M_1M_5$, $ M_3M_5$, $ M_1M_6$, $ M_3M_6$, $ \phi_1q_1\tilde{q}_2$, $ M_3q_2\tilde{q}_2$, $ M_4^2$, $ M_1M_4$, $ M_3M_4$, $ q_1q_2\tilde{q}_1^2$, $ M_5\phi_1q_2^2$, $ M_6\phi_1q_2^2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_1^2$, $ M_1M_3$, $ M_3^2$, $ M_5q_1\tilde{q}_1$, $ M_6q_1\tilde{q}_1$ | $M_4\phi_1q_2^2$ | -2 | t^2.12 + 3*t^2.33 + t^2.7 + 2*t^2.9 + t^3.3 + t^3.47 + t^3.88 + t^4.04 + 2*t^4.25 + 4*t^4.45 + 6*t^4.65 + t^4.82 + 5*t^5.02 + 6*t^5.22 + t^5.39 + 3*t^5.59 + 2*t^5.63 + 4*t^5.8 - 2*t^6. + 2*t^6.17 + 2*t^6.2 + 5*t^6.37 + 4*t^6.57 + t^6.61 + t^6.74 + 8*t^6.78 + 4*t^6.94 + 7*t^6.98 + 6*t^7.14 + 10*t^7.35 + 2*t^7.51 + 8*t^7.55 + 6*t^7.72 - t^7.75 + 8*t^7.92 + 3*t^7.96 + 2*t^8.09 + 4*t^8.12 + 5*t^8.29 - 9*t^8.33 + 10*t^8.49 + t^8.53 + 8*t^8.7 + 2*t^8.86 - 2*t^8.9 + 2*t^8.93 - t^4.55/y - (2*t^6.88)/y + (2*t^7.45)/y + (4*t^7.65)/y + t^7.82/y + (5*t^8.02)/y + (8*t^8.22)/y + t^8.43/y + (3*t^8.59)/y + (3*t^8.63)/y + (4*t^8.8)/y - t^4.55*y - 2*t^6.88*y + 2*t^7.45*y + 4*t^7.65*y + t^7.82*y + 5*t^8.02*y + 8*t^8.22*y + t^8.43*y + 3*t^8.59*y + 3*t^8.63*y + 4*t^8.8*y | g1^5*t^2.12 + (3*t^2.33)/g1^3 + g1^12*t^2.7 + 2*g1^4*t^2.9 + t^3.3/g1^12 + g1^11*t^3.47 + t^3.88/g1^5 + g1^18*t^4.04 + 2*g1^10*t^4.25 + 4*g1^2*t^4.45 + (6*t^4.65)/g1^6 + g1^17*t^4.82 + 5*g1^9*t^5.02 + 6*g1*t^5.22 + g1^24*t^5.39 + 3*g1^16*t^5.59 + (2*t^5.63)/g1^15 + 4*g1^8*t^5.8 - 2*t^6. + 2*g1^23*t^6.17 + (2*t^6.2)/g1^8 + 5*g1^15*t^6.37 + 4*g1^7*t^6.57 + t^6.61/g1^24 + g1^30*t^6.74 + (8*t^6.78)/g1 + 4*g1^22*t^6.94 + (7*t^6.98)/g1^9 + 6*g1^14*t^7.14 + 10*g1^6*t^7.35 + 2*g1^29*t^7.51 + (8*t^7.55)/g1^2 + 6*g1^21*t^7.72 - t^7.75/g1^10 + 8*g1^13*t^7.92 + (3*t^7.96)/g1^18 + 2*g1^36*t^8.09 + 4*g1^5*t^8.12 + 5*g1^28*t^8.29 - (9*t^8.33)/g1^3 + 10*g1^20*t^8.49 + t^8.53/g1^11 + 8*g1^12*t^8.7 + 2*g1^35*t^8.86 - 2*g1^4*t^8.9 + (2*t^8.93)/g1^27 - t^4.55/(g1^2*y) - (2*t^6.88)/(g1^5*y) + (2*g1^2*t^7.45)/y + (4*t^7.65)/(g1^6*y) + (g1^17*t^7.82)/y + (5*g1^9*t^8.02)/y + (8*g1*t^8.22)/y + t^8.43/(g1^7*y) + (3*g1^16*t^8.59)/y + (3*t^8.63)/(g1^15*y) + (4*g1^8*t^8.8)/y - (t^4.55*y)/g1^2 - (2*t^6.88*y)/g1^5 + 2*g1^2*t^7.45*y + (4*t^7.65*y)/g1^6 + g1^17*t^7.82*y + 5*g1^9*t^8.02*y + 8*g1*t^8.22*y + (t^8.43*y)/g1^7 + 3*g1^16*t^8.59*y + (3*t^8.63*y)/g1^15 + 4*g1^8*t^8.8*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1885 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ q_1q_2\tilde{q}_2^2$ | 0.616 | 0.7963 | 0.7736 | [X:[], M:[0.964, 1.108, 0.964, 0.892, 0.777], q:[0.741, 0.295], qb:[0.41, 0.482], phi:[0.518]] | t^2.11 + 2*t^2.33 + t^2.68 + 2*t^2.89 + t^3.32 + t^3.45 + t^3.67 + t^3.89 + t^4.01 + 2*t^4.23 + 3*t^4.45 + 3*t^4.66 + t^4.79 + 4*t^5.01 + 4*t^5.22 + t^5.35 + 3*t^5.57 + t^5.66 + 4*t^5.78 - t^4.55/y - t^4.55*y | detail |