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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
45207 SO5adj1nf2 $M_1\phi_1^2q_1$ + $ M_1q_2^2$ + $ M_2q_2^2$ + $ \phi_1^4q_2$ 1.7803 1.9053 0.9344 [X:[], M:[0.9091, 0.9091], q:[0.3636, 0.5455], qb:[], phi:[0.3636]] [X:[], M:[[0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 18957/10648, c: 2536/1331, M1: 10/11, M2: 10/11, q1: 4/11, q2: 6/11, phi1: 4/11}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1^2$, $ q_1^2$, $ M_1$, $ M_2$, $ q_1q_2$, $ \phi_1^2q_2$, $ \phi_1q_1q_2$, $ \phi_1^4$, $ \phi_1^2q_1^2$, $ q_1^4$, $ M_1\phi_1^2$, $ M_2\phi_1^2$, $ M_1q_1^2$, $ M_2q_1^2$, $ \phi_1^2q_1q_2$, $ q_1^3q_2$, $ M_1^2$, $ M_1M_2$, $ M_2^2$, $ M_2q_1q_2$, $ \phi_1^2q_2^2$, $ q_1^2q_2^2$ $2\phi_1^3q_1q_2$, $ \phi_1^2q_1^2q_2$, $ \phi_1q_1^3q_2$ 3 2*t^2.18 + 3*t^2.73 + 2*t^3.82 + 5*t^4.36 + 7*t^4.91 + 6*t^5.45 + 3*t^6. + 11*t^6.55 + 15*t^7.09 + 15*t^7.64 + 15*t^8.18 + 15*t^8.73 - t^4.09/y - t^5.18/y - t^5.73/y - (3*t^6.27)/y - (3*t^6.82)/y - t^7.36/y - (5*t^8.45)/y - t^4.09*y - t^5.18*y - t^5.73*y - 3*t^6.27*y - 3*t^6.82*y - t^7.36*y - 5*t^8.45*y 2*t^2.18 + 3*t^2.73 + 2*t^3.82 + 5*t^4.36 + 7*t^4.91 + 6*t^5.45 + 3*t^6. + 11*t^6.55 + 15*t^7.09 + 15*t^7.64 + 15*t^8.18 + 15*t^8.73 - t^4.09/y - t^5.18/y - t^5.73/y - (3*t^6.27)/y - (3*t^6.82)/y - t^7.36/y - (5*t^8.45)/y - t^4.09*y - t^5.18*y - t^5.73*y - 3*t^6.27*y - 3*t^6.82*y - t^7.36*y - 5*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
45379 $M_1\phi_1^2q_1$ + $ M_1q_2^2$ + $ M_2q_2^2$ + $ \phi_1^4q_2$ + $ M_3\phi_1^2q_2$ 1.8002 1.9422 0.9269 [X:[], M:[0.9091, 0.9091, 0.7273], q:[0.3636, 0.5455], qb:[], phi:[0.3636]] 3*t^2.18 + 3*t^2.73 + t^3.82 + 8*t^4.36 + 10*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: 38337/21296, c: 20681/10648, M1: 10/11, M2: 10/11, M3: 8/11, q1: 4/11, q2: 6/11, 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
45092 SO5adj1nf2 $M_1\phi_1^2q_1$ + $ M_1q_2^2$ + $ M_2q_2^2$ 1.7923 1.9121 0.9373 [X:[], M:[0.8941, 0.8941], q:[0.4236, 0.5529], qb:[], phi:[0.3412]] t^2.05 + t^2.54 + 2*t^2.68 + t^2.93 + t^3.71 + t^3.95 + 2*t^4.09 + 2*t^4.59 + 2*t^4.73 + 2*t^4.98 + t^5.08 + 2*t^5.22 + 4*t^5.36 + t^5.47 + t^5.61 + t^5.75 + t^5.86 - t^4.02/y - t^5.29/y - t^5.68/y - t^4.02*y - t^5.29*y - t^5.68*y detail