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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
79525 Sp2s2nf1 ${}M_{1}q_{1}q_{2}$ + ${ }M_{1}S_{1}S_{2}$ + ${ }M_{1}M_{2}$ 2.3801 2.5051 0.9501 [X:[], M:[0.8571, 1.1429], q:[0.5714, 0.5714], qb:[], phi:[], S:[0.5714, 0.5714], Sb:[], A:[], Ab:[]] [X:[], M:[[0, 0], [0, 0]], q:[[-1, 0], [1, 0]], qb:[], phi:[], S:[[0, -1], [0, 1]], Sb:[], A:[], Ab:[]] 2 {a: 933/392, c: 491/196, M1: 6/7, M2: 8/7, q1: 4/7, q2: 4/7, S1: 4/7, S2: 4/7}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }S_{1}^{2}$, ${ }S_{1}S_{2}$, ${ }S_{2}^{2}$, ${ }S_{1}^{2}$, ${ }S_{2}^{2}$, ${ }q_{1}q_{2}S_{1}$, ${ }q_{1}^{2}S_{1}$, ${ }q_{2}^{2}S_{1}$, ${ }q_{1}q_{2}S_{2}$, ${ }q_{1}^{2}S_{2}$, ${ }q_{2}^{2}S_{2}$ ${}$ -7 4*t^3.429 + 6*t^5.143 - 7*t^6. + 22*t^6.857 - 14*t^7.714 + 48*t^8.571 - (2*t^4.714)/y + (2*t^7.286)/y - (12*t^8.143)/y - 2*t^4.714*y + 2*t^7.286*y - 12*t^8.143*y 2*t^3.429 + t^3.429/g2^2 + g2^2*t^3.429 + t^5.143/g2 + t^5.143/(g1^2*g2) + (g1^2*t^5.143)/g2 + g2*t^5.143 + (g2*t^5.143)/g1^2 + g1^2*g2*t^5.143 - 3*t^6. - t^6./g1^2 - g1^2*t^6. - t^6./g2^2 - g2^2*t^6. + 8*t^6.857 + t^6.857/g1^2 + g1^2*t^6.857 + (2*t^6.857)/g2^4 + (4*t^6.857)/g2^2 + 4*g2^2*t^6.857 + 2*g2^4*t^6.857 - (3*t^7.714)/g2 - (2*t^7.714)/(g1^2*g2) - (2*g1^2*t^7.714)/g2 - 3*g2*t^7.714 - (2*g2*t^7.714)/g1^2 - 2*g1^2*g2*t^7.714 + 2*t^8.571 + t^8.571/g1^2 + g1^2*t^8.571 + (2*t^8.571)/g2^3 + (2*t^8.571)/(g1^2*g2^3) + (2*g1^2*t^8.571)/g2^3 + (6*t^8.571)/g2 + (5*t^8.571)/(g1^2*g2) + (5*g1^2*t^8.571)/g2 + 6*g2*t^8.571 + (5*g2*t^8.571)/g1^2 + 5*g1^2*g2*t^8.571 + 2*g2^3*t^8.571 + (2*g2^3*t^8.571)/g1^2 + 2*g1^2*g2^3*t^8.571 - t^4.714/(g2*y) - (g2*t^4.714)/y + t^7.286/(g2*y) + (g2*t^7.286)/y - (2*t^8.143)/(g2^3*y) - (4*t^8.143)/(g2*y) - (4*g2*t^8.143)/y - (2*g2^3*t^8.143)/y - (t^4.714*y)/g2 - g2*t^4.714*y + (t^7.286*y)/g2 + g2*t^7.286*y - (2*t^8.143*y)/g2^3 - (4*t^8.143*y)/g2 - 4*g2*t^8.143*y - 2*g2^3*t^8.143*y


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
79488 Sp2s2nf1 ${}M_{1}q_{1}q_{2}$ + ${ }M_{1}S_{1}S_{2}$ 2.3927 2.5266 0.947 [X:[], M:[0.8571], q:[0.5714, 0.5714], qb:[], phi:[], S:[0.5714, 0.5714], Sb:[], A:[], Ab:[]] t^2.571 + 3*t^3.429 + 7*t^5.143 - 4*t^6. - (2*t^4.714)/y - 2*t^4.714*y detail {a: 13131/5488, c: 6933/2744, M1: 6/7, q1: 4/7, q2: 4/7, S1: 4/7, S2: 4/7}