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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
45157 SO5adj1nf2 $q_1^3q_2$ + $ M_1q_2^2$ + $ M_2q_1^2$ + $ M_1\phi_1^2$ 1.7522 1.8544 0.9448 [X:[], M:[1.2727, 0.9091], q:[0.5455, 0.3636], qb:[], phi:[0.3636]] [X:[], M:[[0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 18657/10648, c: 9873/5324, M1: 14/11, M2: 10/11, q1: 6/11, q2: 4/11, phi1: 4/11}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1^2$, $ M_2$, $ q_1q_2$, $ \phi_1^2q_2$, $ M_1$, $ \phi_1^2q_1$, $ \phi_1q_1q_2$, $ \phi_1^4$, $ \phi_1^2q_2^2$, $ M_2\phi_1^2$, $ \phi_1^2q_1q_2$, $ M_2^2$, $ \phi_1^2q_1^2$, $ \phi_1^4q_2$, $ M_2q_1q_2$ $\phi_1^4q_1$, $ M_2\phi_1^2q_2$, $ 2\phi_1^3q_1q_2$, $ \phi_1^2q_1q_2^2$ 4 t^2.18 + 2*t^2.73 + t^3.27 + 3*t^3.82 + 3*t^4.36 + 3*t^4.91 + 4*t^5.45 + 4*t^6. + 7*t^6.55 + 8*t^7.09 + 11*t^7.64 + 12*t^8.18 + 10*t^8.73 - t^4.09/y - t^5.18/y - t^5.73/y - (2*t^6.27)/y - (2*t^6.82)/y - (2*t^7.36)/y - (3*t^7.91)/y - (3*t^8.45)/y - t^4.09*y - t^5.18*y - t^5.73*y - 2*t^6.27*y - 2*t^6.82*y - 2*t^7.36*y - 3*t^7.91*y - 3*t^8.45*y t^2.18 + 2*t^2.73 + t^3.27 + 3*t^3.82 + 3*t^4.36 + 3*t^4.91 + 4*t^5.45 + 4*t^6. + 7*t^6.55 + 8*t^7.09 + 11*t^7.64 + 12*t^8.18 + 10*t^8.73 - t^4.09/y - t^5.18/y - t^5.73/y - (2*t^6.27)/y - (2*t^6.82)/y - (2*t^7.36)/y - (3*t^7.91)/y - (3*t^8.45)/y - t^4.09*y - t^5.18*y - t^5.73*y - 2*t^6.27*y - 2*t^6.82*y - 2*t^7.36*y - 3*t^7.91*y - 3*t^8.45*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
45296 $q_1^3q_2$ + $ M_1q_2^2$ + $ M_2q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2q_2$ 1.7605 1.8684 0.9422 [X:[], M:[1.2727, 0.9091, 0.9091], q:[0.5455, 0.3636], qb:[], phi:[0.3636]] t^2.18 + 3*t^2.73 + 3*t^3.82 + 3*t^4.36 + 4*t^4.91 + 6*t^5.45 + 2*t^6. - t^4.09/y - t^5.18/y - t^5.73/y - t^4.09*y - t^5.18*y - t^5.73*y detail {a: 37491/21296, c: 19895/10648, M1: 14/11, M2: 10/11, M3: 10/11, q1: 6/11, q2: 4/11, phi1: 4/11}


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
45049 SO5adj1nf2 $q_1^3q_2$ + $ M_1q_2^2$ + $ M_2q_1^2$ 1.785 1.8889 0.945 [X:[], M:[1.0422, 0.9859], q:[0.507, 0.4789], qb:[], phi:[0.338]] t^2.03 + 2*t^2.96 + t^3.13 + t^3.46 + t^3.55 + t^3.97 + 2*t^4.06 + t^4.9 + 3*t^4.99 + t^5.07 + t^5.15 + t^5.49 + t^5.58 + 2*t^5.92 - t^4.01/y - t^5.45/y - t^5.54/y - t^4.01*y - t^5.45*y - t^5.54*y detail