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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
79675 Sp2s2nf1 ${}M_{1}S_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{3}S_{2}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{4}S_{1}S_{2}$ 2.3312 2.5114 0.9282 [X:[], M:[0.685, 1.0276, 0.9724, 0.8287], q:[0.4862, 0.4862], qb:[], phi:[], S:[0.6575, 0.5138], Sb:[], A:[], Ab:[]] [X:[], M:[[0, 4], [0, 6], [0, -6], [0, -1]], q:[[-1, -6], [1, 0]], qb:[], phi:[], S:[[0, -2], [0, 3]], Sb:[], A:[], Ab:[]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }M_{4}$, ${ }M_{3}$, ${ }M_{2}$, ${ }M_{1}^{2}$, ${ }q_{1}^{2}S_{2}$, ${ }q_{1}q_{2}S_{2}$, ${ }q_{2}^{2}S_{2}$, ${ }M_{1}M_{4}$, ${ }q_{1}^{2}S_{1}$, ${ }q_{1}q_{2}S_{1}$, ${ }q_{2}^{2}S_{1}$, ${ }M_{1}M_{3}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}^{2}$ ${}q_{1}q_{2}S_{2}^{2}$ -3 t^2.055 + t^2.486 + t^2.917 + t^3.083 + t^4.11 + 3*t^4.459 + t^4.541 + 3*t^4.89 + 2*t^4.972 + t^5.138 + t^5.404 + t^5.835 - 3*t^6. + 3*t^6.165 + 3*t^6.431 + 3*t^6.514 + 2*t^6.596 + t^6.862 + 3*t^6.945 + 4*t^7.028 + t^7.193 + 3*t^7.376 + 3*t^7.459 + 2*t^7.541 + 3*t^7.807 + 3*t^7.89 + 6*t^7.972 - 3*t^8.055 + 3*t^8.221 + t^8.321 + 7*t^8.404 - 4*t^8.486 + 3*t^8.569 + 2*t^8.652 + t^8.752 + 3*t^8.835 + 2*t^8.917 - t^4.541/y - t^4.972/y - t^6.596/y - t^7.028/y - t^7.459/y + t^7.541/y - (2*t^7.624)/y - t^7.89/y + t^7.972/y - (2*t^8.055)/y + t^8.138/y + t^8.404/y - t^8.486/y + t^8.569/y - t^8.652/y - t^8.917/y - t^4.541*y - t^4.972*y - t^6.596*y - t^7.028*y - t^7.459*y + t^7.541*y - 2*t^7.624*y - t^7.89*y + t^7.972*y - 2*t^8.055*y + t^8.138*y + t^8.404*y - t^8.486*y + t^8.569*y - t^8.652*y - t^8.917*y g2^4*t^2.055 + t^2.486/g2 + t^2.917/g2^6 + g2^6*t^3.083 + g2^8*t^4.11 + t^4.459/(g1^2*g2^9) + t^4.459/g2^3 + g1^2*g2^3*t^4.459 + g2^3*t^4.541 + t^4.89/(g1^2*g2^14) + t^4.89/g2^8 + (g1^2*t^4.89)/g2^2 + (2*t^4.972)/g2^2 + g2^10*t^5.138 + t^5.404/g2^7 + t^5.835/g2^12 - t^6. - t^6./(g1^2*g2^6) - g1^2*g2^6*t^6. + 3*g2^12*t^6.165 + t^6.431/(g1^2*g2^11) + t^6.431/g2^5 + g1^2*g2*t^6.431 + t^6.514/(g1^2*g2^5) + g2*t^6.514 + g1^2*g2^7*t^6.514 + 2*g2^7*t^6.596 + t^6.862/g2^10 + t^6.945/(g1^2*g2^10) + t^6.945/g2^4 + g1^2*g2^2*t^6.945 + 4*g2^2*t^7.028 + g2^14*t^7.193 + t^7.376/(g1^2*g2^15) + t^7.376/g2^9 + (g1^2*t^7.376)/g2^3 + (3*t^7.459)/g2^3 + t^7.541/(g1^2*g2^3) + g1^2*g2^9*t^7.541 + t^7.807/(g1^2*g2^20) + t^7.807/g2^14 + (g1^2*t^7.807)/g2^8 + (3*t^7.89)/g2^8 + (2*t^7.972)/(g1^2*g2^8) + (2*t^7.972)/g2^2 + 2*g1^2*g2^4*t^7.972 - t^8.055/(g1^2*g2^2) - g2^4*t^8.055 - g1^2*g2^10*t^8.055 + 3*g2^16*t^8.221 + t^8.321/g2^13 + (2*t^8.404)/(g1^2*g2^13) + (3*t^8.404)/g2^7 + (2*g1^2*t^8.404)/g2 - t^8.486/(g1^2*g2^7) - (2*t^8.486)/g2 - g1^2*g2^5*t^8.486 + t^8.569/(g1^2*g2) + g2^5*t^8.569 + g1^2*g2^11*t^8.569 + 2*g2^11*t^8.652 + t^8.752/g2^18 + t^8.835/(g1^2*g2^18) + t^8.835/g2^12 + (g1^2*t^8.835)/g2^6 + t^8.917/(g1^4*g2^18) + g1^4*g2^6*t^8.917 - (g2^3*t^4.541)/y - t^4.972/(g2^2*y) - (g2^7*t^6.596)/y - (g2^2*t^7.028)/y - t^7.459/(g2^3*y) + (g2^3*t^7.541)/y - (2*g2^9*t^7.624)/y - t^7.89/(g2^8*y) + t^7.972/(g2^2*y) - (2*g2^4*t^8.055)/y + (g2^10*t^8.138)/y + t^8.404/(g2^7*y) - t^8.486/(g2*y) + (g2^5*t^8.569)/y - (g2^11*t^8.652)/y - t^8.917/(g2^6*y) - g2^3*t^4.541*y - (t^4.972*y)/g2^2 - g2^7*t^6.596*y - g2^2*t^7.028*y - (t^7.459*y)/g2^3 + g2^3*t^7.541*y - 2*g2^9*t^7.624*y - (t^7.89*y)/g2^8 + (t^7.972*y)/g2^2 - 2*g2^4*t^8.055*y + g2^10*t^8.138*y + (t^8.404*y)/g2^7 - (t^8.486*y)/g2 + g2^5*t^8.569*y - g2^11*t^8.652*y - (t^8.917*y)/g2^6


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
79599 Sp2s2nf1 ${}M_{1}S_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{3}S_{2}^{2}$ + ${ }M_{2}M_{3}$ 2.3166 2.4859 0.9319 [X:[], M:[0.6834, 1.0251, 0.9749], q:[0.4874, 0.4874], qb:[], phi:[], S:[0.6583, 0.5126], Sb:[], A:[], Ab:[]] t^2.05 + t^2.925 + t^3.075 + t^3.513 + t^4.1 + 3*t^4.462 + 3*t^4.9 + t^4.975 + t^5.126 + t^5.849 - 3*t^6. - t^4.538/y - t^4.975/y - t^4.538*y - t^4.975*y detail