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$a$ =

$c$ =

$\leq a \leq$

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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
8318 G2adj1nf1 $\phi_1^2X_1$ + $ q_1^4$ 1.266 1.3285 0.953 [X:[1.75], M:[], q:[0.5], qb:[], phi:[0.125]] [X:[[0]], M:[], q:[[0]], qb:[], phi:[[0]]] 0 {a: 10371/8192, c: 10883/8192, X1: 7/4, q1: 1/2, phi1: 1/8}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1^6$, $ \phi_1^3q_1$, $ q_1^2$, $ \phi_1^2q_1^2$, $ \phi_1^12$, $ \phi_1^4q_1^2$, $ \phi_1^9q_1$, $ \phi_1^6q_1^2$, $ X_1$, $ \phi_1^3q_1^3$ $\phi_1^8q_1^2$ 1 t^2.25 + t^2.62 + t^3. + t^3.75 + 2*t^4.5 + t^4.88 + 3*t^5.25 + t^5.62 + t^6. + t^6.38 + 4*t^6.75 + t^7.12 + 4*t^7.5 + 2*t^7.88 + 4*t^8.25 + t^8.25/y^2 - t^3.38/y - t^4.88/y - t^5.25/y - t^5.62/y - t^6./y - t^6.38/y - (2*t^7.12)/y - t^7.5/y - (2*t^7.88)/y - t^8.62/y - t^3.38*y - t^4.88*y - t^5.25*y - t^5.62*y - t^6.*y - t^6.38*y - 2*t^7.12*y - t^7.5*y - 2*t^7.88*y - t^8.62*y + t^8.25*y^2 t^2.25 + t^2.62 + t^3. + t^3.75 + 2*t^4.5 + t^4.88 + 3*t^5.25 + t^5.62 + t^6. + t^6.38 + 4*t^6.75 + t^7.12 + 4*t^7.5 + 2*t^7.88 + 4*t^8.25 + t^8.25/y^2 - t^3.38/y - t^4.88/y - t^5.25/y - t^5.62/y - t^6./y - t^6.38/y - (2*t^7.12)/y - t^7.5/y - (2*t^7.88)/y - t^8.62/y - t^3.38*y - t^4.88*y - t^5.25*y - t^5.62*y - t^6.*y - t^6.38*y - 2*t^7.12*y - t^7.5*y - 2*t^7.88*y - t^8.62*y + t^8.25*y^2


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
8336 $\phi_1^2X_1$ + $ q_1^4$ + $ M_1\phi_1^3q_1$ 1.2548 1.3095 0.9582 [X:[1.75], M:[1.125], q:[0.5], qb:[], phi:[0.125]] t^2.25 + t^3. + t^3.38 + t^3.75 + 2*t^4.5 + 2*t^5.25 + t^5.62 + t^6. - t^3.38/y - t^4.88/y - t^5.25/y - t^5.62/y - t^3.38*y - t^4.88*y - t^5.25*y - t^5.62*y detail {a: 20559/16384, c: 21455/16384, X1: 7/4, M1: 9/8, q1: 1/2, phi1: 1/8}
8331 $\phi_1^2X_1$ + $ q_1^4$ + $ M_1\phi_1^6$ 1.2469 1.2938 0.9638 [X:[1.75], M:[1.25], q:[0.5], qb:[], phi:[0.125]] t^2.62 + t^3. + 2*t^3.75 + t^4.5 + 2*t^5.25 + t^5.62 - t^3.38/y - t^4.88/y - t^5.25/y - t^6./y - t^3.38*y - t^4.88*y - t^5.25*y - t^6.*y detail {a: 10215/8192, c: 10599/8192, X1: 7/4, M1: 5/4, q1: 1/2, phi1: 1/8}


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
8309 G2adj1nf1 $\phi_1^2X_1$ 1.3237 1.4166 0.9344 [X:[1.6893], M:[], q:[0.3785], qb:[], phi:[0.1554]] t^2.27 + t^2.53 + t^2.8 + t^3.2 + t^4.14 + t^4.54 + 2*t^4.8 + 3*t^5.07 + t^5.33 + t^5.47 + t^5.59 + t^5.74 - t^3.47/y - t^5.07/y - t^5.33/y - t^5.74/y - t^6./y - t^3.47*y - t^5.07*y - t^5.33*y - t^5.74*y - t^6.*y detail