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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
8670 Sp2adj1nf1 $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ \phi_1^4X_2$ + $ M_2\phi_1^3q_1^2$ + $ M_1M_2$ 0.7816 0.7955 0.9825 [X:[1.7778, 1.5556], M:[1.1111, 0.8889], q:[0.3889, 0.9444], qb:[], phi:[0.1111]] [X:[[0], [0]], M:[[0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 1013/1296, c: 1031/1296, X1: 16/9, X2: 14/9, M1: 10/9, M2: 8/9, q1: 7/18, q2: 17/18, phi1: 1/9}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_2$, $ M_1$, $ q_1q_2$, $ X_2$, $ M_2^2$, $ X_1$ . 0 t^2.67+t^3.33+t^4.+t^4.67+t^5.33+2*t^6.67+3*t^7.33+2*t^8.+t^8.33+t^7.33/y^2-t^3.33/y-t^4./y-t^6./y-t^6.67/y-t^7.33/y-t^8./y-t^8.67/y-t^3.33*y-t^4.*y-t^6.*y-t^6.67*y-t^7.33*y-t^8.*y-t^8.67*y+t^7.33*y^2 t^2.67+t^3.33+t^4.+t^4.67+t^5.33+2*t^6.67+3*t^7.33+2*t^8.+t^8.33+t^7.33/y^2-t^3.33/y-t^4./y-t^6./y-t^6.67/y-t^7.33/y-t^8./y-t^8.67/y-t^3.33*y-t^4.*y-t^6.*y-t^6.67*y-t^7.33*y-t^8.*y-t^8.67*y+t^7.33*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
8836 $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ \phi_1^4X_2$ + $ M_2\phi_1^3q_1^2$ + $ M_1M_2$ + $ M_1M_3$ 0.7917 0.8125 0.9744 [X:[1.7778, 1.5556], M:[1.1111, 0.8889, 0.8889], q:[0.3889, 0.9444], qb:[], phi:[0.1111]] 2*t^2.67+t^4.+t^4.67+3*t^5.33-t^6.-t^3.33/y-t^4./y-(2*t^6.)/y-t^3.33*y-t^4.*y-2*t^6.*y detail {a: 19/24, c: 13/16, X1: 16/9, X2: 14/9, M1: 10/9, M2: 8/9, M3: 8/9, q1: 7/18, q2: 17/18, phi1: 1/9}
8835 $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ \phi_1^4X_2$ + $ M_2\phi_1^3q_1^2$ + $ M_1M_2$ + $ M_2M_3$ 0.7716 0.7785 0.9911 [X:[1.7778, 1.5556], M:[1.1111, 0.8889, 1.1111], q:[0.3889, 0.9444], qb:[], phi:[0.1111]] 2*t^3.33+t^4.+t^4.67-t^6.-t^3.33/y-t^4./y-t^3.33*y-t^4.*y detail {a: 125/162, c: 1009/1296, X1: 16/9, X2: 14/9, M1: 10/9, M2: 8/9, M3: 10/9, q1: 7/18, q2: 17/18, phi1: 1/9}


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
8491 Sp2adj1nf1 $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ \phi_1^4X_2$ + $ M_2\phi_1^3q_1^2$ 0.7976 0.8095 0.9853 [X:[1.8095, 1.619], M:[0.9524, 0.7619], q:[0.4762, 0.9524], qb:[], phi:[0.0952]] t^2.29+t^2.86+t^4.29+t^4.57+t^4.86+t^5.14+t^5.71-t^6.-t^3.29/y-t^3.86/y-t^5.57/y-t^3.29*y-t^3.86*y-t^5.57*y detail {a: 67/84, c: 17/21, X1: 38/21, X2: 34/21, M1: 20/21, M2: 16/21, q1: 10/21, q2: 20/21, phi1: 2/21}