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 |
|---|---|---|---|---|---|---|---|---|---|
| 46448 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2M_5$ | 0.6178 | 0.753 | 0.8204 | [X:[], M:[1.1598, 0.7771, 0.8402, 0.7693, 1.2229], q:[0.3846, 0.4556], qb:[0.8383, 0.7752], phi:[0.3866]] | [X:[], M:[[-3, -3], [2, 4], [3, 3], [-6, -8], [-2, -4]], q:[[-3, -4], [6, 7]], qb:[[1, 0], [0, 1]], phi:[[-1, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ \phi_1^2$, $ M_3$, $ \phi_1q_1^2$, $ M_1$, $ M_5$, $ \phi_1q_1q_2$, $ q_2\tilde{q}_1$, $ \phi_1q_2^2$, $ M_4^2$, $ M_4\phi_1^2$, $ \phi_1^4$, $ \phi_1q_1\tilde{q}_2$, $ M_3M_4$, $ \phi_1q_1\tilde{q}_1$, $ M_3\phi_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ \phi_1q_2\tilde{q}_1$, $ M_4\phi_1q_1^2$, $ M_1M_4$, $ \phi_1^3q_1^2$, $ M_4M_5$, $ M_5\phi_1^2$, $ M_4\phi_1q_1q_2$ | $\phi_1^3q_1q_2$ | -1 | t^2.31 + t^2.32 + t^2.52 + t^3.47 + t^3.48 + t^3.67 + t^3.68 + t^3.88 + t^3.89 + t^4.62 + t^4.63 + t^4.64 + t^4.83 + 2*t^4.84 + t^5.04 + t^5.78 + t^5.79 + t^5.98 + 2*t^5.99 - t^6. - t^6.01 + 2*t^6.19 + 2*t^6.2 + t^6.4 + t^6.41 + t^6.92 + 2*t^6.94 + t^6.95 + t^6.96 + 2*t^7.14 + 2*t^7.15 - t^7.17 + t^7.34 + 2*t^7.35 + t^7.36 - t^7.37 + t^7.55 + 2*t^7.56 + t^7.76 + t^7.77 + t^7.79 + t^8.08 + t^8.1 + t^8.28 + 2*t^8.3 - t^8.31 - 2*t^8.32 - t^8.33 + 2*t^8.5 + 3*t^8.51 - 2*t^8.52 - 2*t^8.53 + 2*t^8.71 + 2*t^8.72 + t^8.92 + t^8.93 - t^4.16/y - t^6.47/y - t^6.48/y + t^7.63/y + t^7.83/y + (2*t^7.84)/y + t^7.85/y + t^8.79/y + t^8.98/y + (3*t^8.99)/y - t^4.16*y - t^6.47*y - t^6.48*y + t^7.63*y + t^7.83*y + 2*t^7.84*y + t^7.85*y + t^8.79*y + t^8.98*y + 3*t^8.99*y | t^2.31/(g1^6*g2^8) + t^2.32/(g1^2*g2^2) + g1^3*g2^3*t^2.52 + t^3.47/(g1^7*g2^9) + t^3.48/(g1^3*g2^3) + t^3.67/(g1^2*g2^4) + g1^2*g2^2*t^3.68 + g1^7*g2^7*t^3.88 + g1^11*g2^13*t^3.89 + t^4.62/(g1^12*g2^16) + t^4.63/(g1^8*g2^10) + t^4.64/(g1^4*g2^4) + t^4.83/(g1^3*g2^5) + 2*g1*g2*t^4.84 + g1^6*g2^6*t^5.04 + t^5.78/(g1^13*g2^17) + t^5.79/(g1^9*g2^11) + t^5.98/(g1^8*g2^12) + (2*t^5.99)/(g1^4*g2^6) - t^6. - g1^4*g2^6*t^6.01 + (2*g1*t^6.19)/g2 + 2*g1^5*g2^5*t^6.2 + g1^10*g2^10*t^6.4 + g1^14*g2^16*t^6.41 + t^6.92/(g1^18*g2^24) + (2*t^6.94)/(g1^14*g2^18) + t^6.95/(g1^10*g2^12) + t^6.96/(g1^6*g2^6) + (2*t^7.14)/(g1^9*g2^13) + (2*t^7.15)/(g1^5*g2^7) - g1^3*g2^5*t^7.17 + t^7.34/(g1^4*g2^8) + (2*t^7.35)/g2^2 + g1^4*g2^4*t^7.36 - g1^8*g2^10*t^7.37 + g1^5*g2^3*t^7.55 + 2*g1^9*g2^9*t^7.56 + g1^14*g2^14*t^7.76 + g1^18*g2^20*t^7.77 + g1^22*g2^26*t^7.79 + t^8.08/(g1^19*g2^25) + t^8.1/(g1^15*g2^19) + t^8.28/(g1^14*g2^20) + (2*t^8.3)/(g1^10*g2^14) - t^8.31/(g1^6*g2^8) - (2*t^8.32)/(g1^2*g2^2) - g1^2*g2^4*t^8.33 + (2*t^8.5)/(g1^5*g2^9) + (3*t^8.51)/(g1*g2^3) - 2*g1^3*g2^3*t^8.52 - 2*g1^7*g2^9*t^8.53 + 2*g1^4*g2^2*t^8.71 + 2*g1^8*g2^8*t^8.72 + g1^13*g2^13*t^8.92 + g1^17*g2^19*t^8.93 - t^4.16/(g1*g2*y) - t^6.47/(g1^7*g2^9*y) - t^6.48/(g1^3*g2^3*y) + t^7.63/(g1^8*g2^10*y) + t^7.83/(g1^3*g2^5*y) + (2*g1*g2*t^7.84)/y + (g1^5*g2^7*t^7.85)/y + t^8.79/(g1^9*g2^11*y) + t^8.98/(g1^8*g2^12*y) + (3*t^8.99)/(g1^4*g2^6*y) - (t^4.16*y)/(g1*g2) - (t^6.47*y)/(g1^7*g2^9) - (t^6.48*y)/(g1^3*g2^3) + (t^7.63*y)/(g1^8*g2^10) + (t^7.83*y)/(g1^3*g2^5) + 2*g1*g2*t^7.84*y + g1^5*g2^7*t^7.85*y + (t^8.79*y)/(g1^9*g2^11) + (t^8.98*y)/(g1^8*g2^12) + (3*t^8.99*y)/(g1^4*g2^6) |
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 |
|---|---|---|---|---|---|---|---|---|
| 48159 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2M_5$ + $ M_6\phi_1q_1^2$ | 0.6327 | 0.7781 | 0.8131 | [X:[], M:[1.1632, 0.7448, 0.8368, 0.8061, 1.2552, 0.8061], q:[0.4031, 0.4337], qb:[0.8521, 0.7601], phi:[0.3877]] | t^2.33 + 2*t^2.42 + t^2.51 + t^3.49 + t^3.67 + 2*t^3.77 + t^3.86 + t^4.65 + 2*t^4.74 + 5*t^4.84 + 2*t^4.93 + t^5.02 - t^6. - t^4.16/y - t^4.16*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46225 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ | 0.6366 | 0.7855 | 0.8105 | [X:[], M:[1.1465, 0.7368, 0.8535, 0.7919], q:[0.396, 0.4575], qb:[0.8673, 0.7506], phi:[0.3822]] | t^2.21 + t^2.29 + t^2.38 + t^2.56 + t^3.44 + t^3.52 + t^3.71 + t^3.89 + t^3.97 + t^4.42 + t^4.5 + 2*t^4.59 + t^4.67 + t^4.75 + t^4.77 + 2*t^4.85 + t^4.94 + t^5.12 + t^5.65 + t^5.73 + t^5.82 + t^5.9 - t^6. - t^4.15/y - t^4.15*y | detail |