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$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

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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
45515 SO5adj1nf2 $M_1q_1q_2$ + $ M_2\phi_1^2q_1$ + $ M_3q_2^2$ + $ M_4\phi_1q_1q_2$ + $ M_3q_1^2$ + $ M_5q_1^2$ 1.8199 1.9527 0.932 [X:[], M:[1.023, 0.8295, 1.023, 0.682, 1.023], q:[0.4885, 0.4885], qb:[], phi:[0.341]] [X:[], M:[[-6], [1], [-6], [-4], [-6]], q:[[3], [3]], qb:[], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_4$, $ \phi_1^2$, $ M_2$, $ M_1$, $ M_3$, $ M_5$, $ \phi_1^2q_2$, $ M_4^2$, $ M_4\phi_1^2$, $ \phi_1^4$, $ M_2M_4$, $ M_2\phi_1^2$, $ M_2^2$, $ \phi_1^2q_1^2$, $ \phi_1^2q_1q_2$, $ \phi_1^2q_2^2$, $ M_1M_4$, $ M_3M_4$, $ M_4M_5$, $ M_1\phi_1^2$, $ M_3\phi_1^2$, $ M_5\phi_1^2$, $ M_1M_2$, $ M_2M_3$, $ M_2M_5$, $ M_4\phi_1^2q_2$, $ \phi_1^4q_2$ $M_2\phi_1^2q_2$, $ \phi_1^3q_1q_2$ -2 2*t^2.05 + t^2.49 + 3*t^3.07 + t^3.51 + 4*t^4.09 + 2*t^4.53 + 4*t^4.98 + 6*t^5.11 + 5*t^5.56 - 2*t^6. + 12*t^6.14 + 5*t^6.58 + 6*t^7.02 + 12*t^7.16 + 4*t^7.47 + 10*t^7.6 - t^7.91 + 5*t^8.05 + 21*t^8.18 - t^8.49 + 14*t^8.63 - 3*t^8.93 - t^4.02/y - (2*t^5.49)/y - (3*t^6.07)/y - t^6.51/y - (2*t^7.09)/y - (3*t^7.53)/y - t^7.98/y - (2*t^8.56)/y - t^4.02*y - 2*t^5.49*y - 3*t^6.07*y - t^6.51*y - 2*t^7.09*y - 3*t^7.53*y - t^7.98*y - 2*t^8.56*y (2*t^2.05)/g1^4 + g1*t^2.49 + (3*t^3.07)/g1^6 + t^3.51/g1 + (4*t^4.09)/g1^8 + (2*t^4.53)/g1^3 + 4*g1^2*t^4.98 + (6*t^5.11)/g1^10 + (5*t^5.56)/g1^5 - 2*t^6. + (12*t^6.14)/g1^12 + (5*t^6.58)/g1^7 + (6*t^7.02)/g1^2 + (12*t^7.16)/g1^14 + 4*g1^3*t^7.47 + (10*t^7.6)/g1^9 - g1^8*t^7.91 + (5*t^8.05)/g1^4 + (21*t^8.18)/g1^16 - g1*t^8.49 + (14*t^8.63)/g1^11 - 3*g1^6*t^8.93 - t^4.02/(g1^2*y) - (2*g1*t^5.49)/y - (3*t^6.07)/(g1^6*y) - t^6.51/(g1*y) - (2*t^7.09)/(g1^8*y) - (3*t^7.53)/(g1^3*y) - (g1^2*t^7.98)/y - (2*t^8.56)/(g1^5*y) - (t^4.02*y)/g1^2 - 2*g1*t^5.49*y - (3*t^6.07*y)/g1^6 - (t^6.51*y)/g1 - (2*t^7.09*y)/g1^8 - (3*t^7.53*y)/g1^3 - g1^2*t^7.98*y - (2*t^8.56*y)/g1^5


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
45277 SO5adj1nf2 $M_1q_1q_2$ + $ M_2\phi_1^2q_1$ + $ M_3q_2^2$ + $ M_4\phi_1q_1q_2$ + $ M_3q_1^2$ 1.8233 1.9562 0.9321 [X:[], M:[1.0494, 0.8251, 1.0494, 0.6996], q:[0.4753, 0.4753], qb:[], phi:[0.3498]] 2*t^2.1 + t^2.48 + t^2.85 + 2*t^3.15 + t^3.52 + 4*t^4.2 + 2*t^4.57 + 6*t^4.95 + 4*t^5.25 + t^5.33 + 4*t^5.62 + t^5.7 - t^4.05/y - (2*t^5.48)/y - t^4.05*y - 2*t^5.48*y detail