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 |
|---|---|---|---|---|---|---|---|---|---|
| 46864 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_2\phi_1^2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_2$ + $ M_5\phi_1q_2\tilde{q}_1$ | 0.6262 | 0.8137 | 0.7696 | [X:[], M:[0.9849, 0.9849, 1.0452, 0.7914, 0.7312], q:[0.7462, 0.2688], qb:[0.4925, 0.4623], phi:[0.5075]] | [X:[], M:[[4], [4], [-12], [-11], [5]], q:[[1], [-5]], qb:[[2], [10]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ M_4$, $ M_1$, $ M_2$, $ M_3$, $ \phi_1q_2^2$, $ q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_5^2$, $ M_5q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_5q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_4M_5$, $ \phi_1q_1q_2$, $ q_2^2\tilde{q}_1^2$, $ M_4q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_1$, $ M_4^2$, $ M_1M_5$, $ M_2M_5$, $ \phi_1q_1\tilde{q}_2$, $ M_2q_2\tilde{q}_2$, $ \phi_1q_1\tilde{q}_1$, $ M_2q_2\tilde{q}_1$, $ M_1M_4$, $ M_2M_4$, $ M_3M_5$, $ M_5\phi_1q_2^2$, $ M_3q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_1$, $ M_3M_4$, $ M_4\phi_1q_2^2$, $ M_1^2$, $ M_1M_2$, $ M_2^2$, $ M_5q_1\tilde{q}_1$, $ M_5\phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_2^2$ | . | -2 | 2*t^2.19 + t^2.28 + t^2.37 + 2*t^2.95 + 2*t^3.14 + 2*t^3.72 + t^4.3 + 4*t^4.39 + 3*t^4.48 + 3*t^4.57 + t^4.66 + t^4.75 + 4*t^5.15 + 2*t^5.24 + 5*t^5.33 + t^5.42 + 2*t^5.51 + 5*t^5.91 - 2*t^6. + 3*t^6.09 + 3*t^6.27 + 2*t^6.49 + 5*t^6.58 + 7*t^6.67 + 3*t^6.76 + 5*t^6.85 + 2*t^6.94 + t^7.03 + t^7.12 + t^7.25 + 6*t^7.34 + 5*t^7.43 + 7*t^7.52 + 3*t^7.61 + 6*t^7.7 + t^7.79 + 2*t^7.88 + t^8.01 + 6*t^8.1 - 4*t^8.19 + 3*t^8.28 - 3*t^8.37 + 7*t^8.46 + t^8.56 + t^8.59 + 3*t^8.65 + 4*t^8.68 + 7*t^8.77 + 11*t^8.86 - 2*t^8.95 - t^4.52/y - t^6.72/y - t^6.9/y + (2*t^7.39)/y + t^7.48/y + (3*t^7.57)/y + (5*t^8.15)/y + (2*t^8.24)/y + (7*t^8.33)/y + (2*t^8.42)/y + (2*t^8.51)/y + (4*t^8.91)/y - t^4.52*y - t^6.72*y - t^6.9*y + 2*t^7.39*y + t^7.48*y + 3*t^7.57*y + 5*t^8.15*y + 2*t^8.24*y + 7*t^8.33*y + 2*t^8.42*y + 2*t^8.51*y + 4*t^8.91*y | 2*g1^5*t^2.19 + t^2.28/g1^3 + t^2.37/g1^11 + 2*g1^4*t^2.95 + (2*t^3.14)/g1^12 + 2*g1^3*t^3.72 + g1^18*t^4.3 + 4*g1^10*t^4.39 + 3*g1^2*t^4.48 + (3*t^4.57)/g1^6 + t^4.66/g1^14 + t^4.75/g1^22 + 4*g1^9*t^5.15 + 2*g1*t^5.24 + (5*t^5.33)/g1^7 + t^5.42/g1^15 + (2*t^5.51)/g1^23 + 5*g1^8*t^5.91 - 2*t^6. + (3*t^6.09)/g1^8 + (3*t^6.27)/g1^24 + 2*g1^23*t^6.49 + 5*g1^15*t^6.58 + 7*g1^7*t^6.67 + (3*t^6.76)/g1 + (5*t^6.85)/g1^9 + (2*t^6.94)/g1^17 + t^7.03/g1^25 + t^7.12/g1^33 + g1^22*t^7.25 + 6*g1^14*t^7.34 + 5*g1^6*t^7.43 + (7*t^7.52)/g1^2 + (3*t^7.61)/g1^10 + (6*t^7.7)/g1^18 + t^7.79/g1^26 + (2*t^7.88)/g1^34 + g1^21*t^8.01 + 6*g1^13*t^8.1 - 4*g1^5*t^8.19 + (3*t^8.28)/g1^3 - (3*t^8.37)/g1^11 + (7*t^8.46)/g1^19 + t^8.56/g1^27 + g1^36*t^8.59 + (3*t^8.65)/g1^35 + 4*g1^28*t^8.68 + 7*g1^20*t^8.77 + 11*g1^12*t^8.86 - 2*g1^4*t^8.95 - t^4.52/(g1^2*y) - (g1^3*t^6.72)/y - t^6.9/(g1^13*y) + (2*g1^10*t^7.39)/y + (g1^2*t^7.48)/y + (3*t^7.57)/(g1^6*y) + (5*g1^9*t^8.15)/y + (2*g1*t^8.24)/y + (7*t^8.33)/(g1^7*y) + (2*t^8.42)/(g1^15*y) + (2*t^8.51)/(g1^23*y) + (4*g1^8*t^8.91)/y - (t^4.52*y)/g1^2 - g1^3*t^6.72*y - (t^6.9*y)/g1^13 + 2*g1^10*t^7.39*y + g1^2*t^7.48*y + (3*t^7.57*y)/g1^6 + 5*g1^9*t^8.15*y + 2*g1*t^8.24*y + (7*t^8.33*y)/g1^7 + (2*t^8.42*y)/g1^15 + (2*t^8.51*y)/g1^23 + 4*g1^8*t^8.91*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46598 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_2\phi_1^2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_2$ | 0.6065 | 0.7774 | 0.7802 | [X:[], M:[0.9872, 0.9872, 1.0385, 0.7853], q:[0.7468, 0.266], qb:[0.4936, 0.4679], phi:[0.5064]] | t^2.2 + t^2.28 + t^2.36 + 2*t^2.96 + 2*t^3.12 + 2*t^3.72 + t^3.8 + t^4.33 + 2*t^4.4 + 2*t^4.48 + 2*t^4.56 + t^4.63 + t^4.71 + 2*t^5.16 + 2*t^5.24 + 3*t^5.32 + t^5.39 + 2*t^5.47 + 3*t^5.92 - t^6. - t^4.52/y - t^4.52*y | detail |