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$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





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.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
45121 SO5adj1nf2 $M_1\phi_1^2q_1$ + $ M_2q_2^2$ + $ M_3\phi_1^2$ + $ M_4\phi_1^2q_2$ 1.8059 1.9216 0.9398 [X:[], M:[0.8374, 1.0503, 1.2749, 0.8], q:[0.4374, 0.4749], qb:[], phi:[0.3626]] [X:[], M:[[-1, 2], [0, -6], [2, 2], [2, -1]], q:[[3, 0], [0, 3]], qb:[], phi:[[-1, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_4$, $ M_1$, $ q_1^2$, $ q_1q_2$, $ M_2$, $ M_3$, $ \phi_1q_1q_2$, $ \phi_1^4$, $ M_4^2$, $ \phi_1^2q_1^2$, $ M_1M_4$, $ \phi_1^2q_1q_2$, $ M_4q_1^2$, $ M_1^2$, $ \phi_1^2q_2^2$, $ M_1q_1^2$, $ M_4q_1q_2$, $ q_1^4$, $ M_1q_1q_2$, $ q_1^3q_2$, $ q_1^2q_2^2$, $ M_2M_4$, $ M_1M_2$, $ M_2q_1^2$ $\phi_1^3q_1q_2$ -1 t^2.4 + t^2.51 + t^2.62 + t^2.74 + t^3.15 + 2*t^3.82 + t^4.35 + 2*t^4.8 + 2*t^4.91 + 3*t^5.02 + 2*t^5.14 + 2*t^5.25 + t^5.36 + t^5.47 + t^5.55 + t^5.66 + t^5.78 - t^6. - t^6.11 + 2*t^6.22 + t^6.3 + 2*t^6.34 + 2*t^6.45 + 2*t^6.56 + 2*t^6.98 + t^7.2 + 3*t^7.31 + 5*t^7.42 + t^7.5 + 6*t^7.54 + 7*t^7.65 + 4*t^7.76 + 3*t^7.87 + 2*t^7.95 + 2*t^7.99 + t^8.06 + t^8.1 + 4*t^8.18 + t^8.21 - t^8.4 - 3*t^8.51 + t^8.62 + 2*t^8.7 + t^8.74 + t^8.81 + 4*t^8.85 + t^8.93 + 4*t^8.96 - t^4.09/y - t^5.4/y - t^5.51/y - t^6.26/y - t^6.49/y - t^6.6/y - t^6.71/y - t^6.82/y - t^7.24/y - t^7.8/y - (2*t^7.91)/y - t^8.02/y + t^8.36/y - t^8.44/y + t^8.78/y - t^8.89/y - t^4.09*y - t^5.4*y - t^5.51*y - t^6.26*y - t^6.49*y - t^6.6*y - t^6.71*y - t^6.82*y - t^7.24*y - t^7.8*y - 2*t^7.91*y - t^8.02*y + t^8.36*y - t^8.44*y + t^8.78*y - t^8.89*y (g1^2*t^2.4)/g2 + (g2^2*t^2.51)/g1 + g1^6*t^2.62 + g1^3*g2^3*t^2.74 + t^3.15/g2^6 + 2*g1^2*g2^2*t^3.82 + t^4.35/(g1^4*g2^4) + (2*g1^4*t^4.8)/g2^2 + 2*g1*g2*t^4.91 + (g1^8*t^5.02)/g2 + (2*g2^4*t^5.02)/g1^2 + 2*g1^5*g2^2*t^5.14 + g1^12*t^5.25 + g1^2*g2^5*t^5.25 + g1^9*g2^3*t^5.36 + g1^6*g2^6*t^5.47 + (g1^2*t^5.55)/g2^7 + t^5.66/(g1*g2^4) + (g1^6*t^5.78)/g2^6 - t^6. - (g2^3*t^6.11)/g1^3 + 2*g1^4*g2*t^6.22 + t^6.3/g2^12 + 2*g1*g2^4*t^6.34 + 2*g1^8*g2^2*t^6.45 + 2*g1^5*g2^5*t^6.56 + (2*g1^2*t^6.98)/g2^4 + (2*g1^6*t^7.2)/g2^3 - (g2^2*t^7.2)/g1^4 + 3*g1^3*t^7.31 + (2*g1^10*t^7.42)/g2^2 + 3*g2^3*t^7.42 + t^7.5/(g1^4*g2^10) + 4*g1^7*g2*t^7.54 + (2*g2^6*t^7.54)/g1^3 + (g1^14*t^7.65)/g2 + 6*g1^4*g2^4*t^7.65 + 2*g1^11*g2^2*t^7.76 + 2*g1*g2^7*t^7.76 + g1^18*t^7.87 + 2*g1^8*g2^5*t^7.87 + (2*g1^4*t^7.95)/g2^8 + g1^15*g2^3*t^7.99 + g1^5*g2^8*t^7.99 + (g1*t^8.06)/g2^5 + g1^12*g2^6*t^8.1 + (g1^8*t^8.18)/g2^7 + (3*t^8.18)/(g1^2*g2^2) + g1^9*g2^9*t^8.21 + (g1^5*t^8.29)/g2^4 - (g2*t^8.29)/g1^5 + (g1^12*t^8.4)/g2^6 - (2*g1^2*t^8.4)/g2 - (3*g2^2*t^8.51)/g1 + 2*g1^6*t^8.62 - (g2^5*t^8.62)/g1^4 + (g1^2*t^8.7)/g2^13 + t^8.7/(g1^8*g2^8) + g1^3*g2^3*t^8.74 + t^8.81/(g1*g2^10) + 2*g1^10*g2*t^8.85 + 2*g2^6*t^8.85 + (g1^6*t^8.93)/g2^12 + 4*g1^7*g2^4*t^8.96 - t^4.09/(g1*g2*y) - (g1^2*t^5.4)/(g2*y) - (g2^2*t^5.51)/(g1*y) - t^6.26/(g1^3*g2^3*y) - (g1*t^6.49)/(g2^2*y) - (g2*t^6.6)/(g1^2*y) - (g1^5*t^6.71)/(g2*y) - (g1^2*g2^2*t^6.82)/y - t^7.24/(g1*g2^7*y) - (g1^4*t^7.8)/(g2^2*y) - (2*g1*g2*t^7.91)/y - (g2^4*t^8.02)/(g1^2*y) + (g1^9*g2^3*t^8.36)/y - t^8.44/(g1^5*g2^5*y) + (g1^6*t^8.78)/(g2^6*y) - (g1^3*t^8.89)/(g2^3*y) - (t^4.09*y)/(g1*g2) - (g1^2*t^5.4*y)/g2 - (g2^2*t^5.51*y)/g1 - (t^6.26*y)/(g1^3*g2^3) - (g1*t^6.49*y)/g2^2 - (g2*t^6.6*y)/g1^2 - (g1^5*t^6.71*y)/g2 - g1^2*g2^2*t^6.82*y - (t^7.24*y)/(g1*g2^7) - (g1^4*t^7.8*y)/g2^2 - 2*g1*g2*t^7.91*y - (g2^4*t^8.02*y)/g1^2 + g1^9*g2^3*t^8.36*y - (t^8.44*y)/(g1^5*g2^5) + (g1^6*t^8.78*y)/g2^6 - (g1^3*t^8.89*y)/g2^3


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore 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.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
45066 SO5adj1nf2 $M_1\phi_1^2q_1$ + $ M_2q_2^2$ + $ M_3\phi_1^2$ 1.7896 1.8921 0.9458 [X:[], M:[0.8313, 1.0608, 1.2766], q:[0.4452, 0.4696], qb:[], phi:[0.3617]] t^2.49 + t^2.67 + t^2.74 + t^3.18 + t^3.58 + 2*t^3.83 + t^4.34 + t^4.84 + t^4.91 + 2*t^4.99 + t^5.17 + t^5.24 + t^5.34 + t^5.42 + t^5.49 + t^5.68 + t^5.85 - t^6. - t^4.09/y - t^5.42/y - t^5.49/y - t^4.09*y - t^5.42*y - t^5.49*y detail