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 |
|---|---|---|---|---|---|---|---|---|---|
| 55107 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_1$ + $ M_6\tilde{q}_1\tilde{q}_2$ | 0.6432 | 0.8457 | 0.7606 | [X:[], M:[0.9963, 1.0037, 0.7601, 0.7454, 0.7527, 1.011], q:[0.7491, 0.2546], qb:[0.4982, 0.4909], phi:[0.5018]] | [X:[], M:[[4], [-4], [-11], [5], [-3], [-12]], q:[[1], [-5]], qb:[[2], [10]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ q_2\tilde{q}_2$, $ M_5$, $ q_2\tilde{q}_1$, $ M_3$, $ M_2$, $ \phi_1^2$, $ M_6$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_4^2$, $ M_4q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_4M_5$, $ M_4q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_5q_2\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_3M_4$, $ M_5^2$, $ \phi_1q_1q_2$, $ M_5q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_3q_2\tilde{q}_2$, $ M_3M_5$, $ M_3q_2\tilde{q}_1$, $ M_3^2$, $ M_2M_4$, $ M_4\phi_1^2$, $ \phi_1q_1\tilde{q}_1$, $ M_2q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_2M_5$, $ M_4M_6$, $ M_5\phi_1^2$, $ M_4\phi_1q_2^2$, $ M_2q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_2M_3$, $ M_5M_6$, $ M_3\phi_1^2$, $ M_5\phi_1q_2^2$, $ M_6q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_3M_6$, $ M_3\phi_1q_2^2$ | $M_5\phi_1q_2\tilde{q}_2$ | -2 | 2*t^2.24 + 2*t^2.26 + t^2.28 + 2*t^3.01 + 2*t^3.03 + t^3.74 + t^4.45 + 4*t^4.47 + 5*t^4.49 + 5*t^4.52 + 2*t^4.54 + t^4.56 + 4*t^5.25 + 7*t^5.27 + 5*t^5.29 + 2*t^5.31 - 2*t^6. + t^6.02 + 4*t^6.04 + 3*t^6.07 + 2*t^6.69 + 6*t^6.71 + 7*t^6.73 + 10*t^6.75 + 8*t^6.77 + 4*t^6.8 + 2*t^6.82 + t^6.84 - t^7.44 + 5*t^7.48 + 11*t^7.51 + 14*t^7.53 + 11*t^7.55 + 5*t^7.57 + 2*t^7.59 - 4*t^8.21 - 10*t^8.24 - 5*t^8.26 + 4*t^8.28 + 11*t^8.3 + 8*t^8.32 + 3*t^8.35 + t^8.9 + 4*t^8.92 + 9*t^8.95 + 9*t^8.97 + 9*t^8.99 - t^4.51/y - t^6.74/y - t^6.76/y - t^6.79/y + (2*t^7.47)/y + (5*t^7.49)/y + (2*t^7.52)/y + t^7.54/y + t^8.23/y + (5*t^8.25)/y + (9*t^8.27)/y + (6*t^8.29)/y + (2*t^8.31)/y + t^8.98/y - t^4.51*y - t^6.74*y - t^6.76*y - t^6.79*y + 2*t^7.47*y + 5*t^7.49*y + 2*t^7.52*y + t^7.54*y + t^8.23*y + 5*t^8.25*y + 9*t^8.27*y + 6*t^8.29*y + 2*t^8.31*y + t^8.98*y | 2*g1^5*t^2.24 + (2*t^2.26)/g1^3 + t^2.28/g1^11 + (2*t^3.01)/g1^4 + (2*t^3.03)/g1^12 + g1^3*t^3.74 + g1^18*t^4.45 + 4*g1^10*t^4.47 + 5*g1^2*t^4.49 + (5*t^4.52)/g1^6 + (2*t^4.54)/g1^14 + t^4.56/g1^22 + 4*g1*t^5.25 + (7*t^5.27)/g1^7 + (5*t^5.29)/g1^15 + (2*t^5.31)/g1^23 - 2*t^6. + t^6.02/g1^8 + (4*t^6.04)/g1^16 + (3*t^6.07)/g1^24 + 2*g1^23*t^6.69 + 6*g1^15*t^6.71 + 7*g1^7*t^6.73 + (10*t^6.75)/g1 + (8*t^6.77)/g1^9 + (4*t^6.8)/g1^17 + (2*t^6.82)/g1^25 + t^6.84/g1^33 - g1^22*t^7.44 + 5*g1^6*t^7.48 + (11*t^7.51)/g1^2 + (14*t^7.53)/g1^10 + (11*t^7.55)/g1^18 + (5*t^7.57)/g1^26 + (2*t^7.59)/g1^34 - 4*g1^13*t^8.21 - 10*g1^5*t^8.24 - (5*t^8.26)/g1^3 + (4*t^8.28)/g1^11 + (11*t^8.3)/g1^19 + (8*t^8.32)/g1^27 + (3*t^8.35)/g1^35 + g1^36*t^8.9 + 4*g1^28*t^8.92 + 9*g1^20*t^8.95 + 9*g1^12*t^8.97 + 9*g1^4*t^8.99 - t^4.51/(g1^2*y) - (g1^3*t^6.74)/y - t^6.76/(g1^5*y) - t^6.79/(g1^13*y) + (2*g1^10*t^7.47)/y + (5*g1^2*t^7.49)/y + (2*t^7.52)/(g1^6*y) + t^7.54/(g1^14*y) + (g1^9*t^8.23)/y + (5*g1*t^8.25)/y + (9*t^8.27)/(g1^7*y) + (6*t^8.29)/(g1^15*y) + (2*t^8.31)/(g1^23*y) + (g1^8*t^8.98)/y - (t^4.51*y)/g1^2 - g1^3*t^6.74*y - (t^6.76*y)/g1^5 - (t^6.79*y)/g1^13 + 2*g1^10*t^7.47*y + 5*g1^2*t^7.49*y + (2*t^7.52*y)/g1^6 + (t^7.54*y)/g1^14 + g1^9*t^8.23*y + 5*g1*t^8.25*y + (9*t^8.27*y)/g1^7 + (6*t^8.29*y)/g1^15 + (2*t^8.31*y)/g1^23 + g1^8*t^8.98*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46922 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_1$ | 0.6462 | 0.8496 | 0.7606 | [X:[], M:[0.9822, 1.0178, 0.799, 0.7277, 0.7634], q:[0.7455, 0.2723], qb:[0.4911, 0.4555], phi:[0.5089]] | 2*t^2.18 + 2*t^2.29 + t^2.4 + t^2.84 + 2*t^3.05 + t^3.16 + t^3.71 + t^4.26 + 4*t^4.37 + 5*t^4.47 + 5*t^4.58 + 2*t^4.69 + t^4.79 + 2*t^5.02 + 2*t^5.13 + 5*t^5.24 + 5*t^5.34 + 3*t^5.45 + t^5.56 + t^5.68 + 2*t^5.89 - t^6. - t^4.53/y - t^4.53*y | detail |