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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
45160 SO5adj1nf2 $q_1^3q_2$ + $ q_2^2$ + $ \phi_1^2X_1$ + $ q_1^2X_2$ + $ M_1\phi_1^4$ + $ M_2\phi_1^2q_1$ 1.1242 1.1173 1.0062 [X:[1.5556, 1.3333], M:[1.1111, 1.2222], q:[0.3333, 1.0], qb:[], phi:[0.2222]] [X:[[0], [0]], M:[[0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 1457/1296, c: 181/162, X1: 14/9, X2: 4/3, M1: 10/9, M2: 11/9, q1: 1/3, q2: 1, phi1: 2/9}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ \phi_1^2q_1^2$, $ M_2$, $ q_1q_2$, $ X_2$, $ \phi_1q_1q_2$, $ X_1$ $\phi_1^3q_1q_2$ -1 2*t^3.33 + t^3.67 + t^4. + t^4.67 - t^6. - t^6.33 + 3*t^6.67 + 2*t^7. + 3*t^7.33 + t^7.67 + 2*t^8. + 2*t^8.33 + 2*t^8.67 + t^8.33/y^2 + t^8.67/y^2 - t^3.67/y - t^4.67/y - t^5./y - t^7./y - t^7.67/y - (2*t^8.)/y - (2*t^8.33)/y - t^8.67/y - t^3.67*y - t^4.67*y - t^5.*y - t^7.*y - t^7.67*y - 2*t^8.*y - 2*t^8.33*y - t^8.67*y + t^8.33*y^2 + t^8.67*y^2 2*t^3.33 + t^3.67 + t^4. + t^4.67 - t^6. - t^6.33 + 3*t^6.67 + 2*t^7. + 3*t^7.33 + t^7.67 + 2*t^8. + 2*t^8.33 + 2*t^8.67 + t^8.33/y^2 + t^8.67/y^2 - t^3.67/y - t^4.67/y - t^5./y - t^7./y - t^7.67/y - (2*t^8.)/y - (2*t^8.33)/y - t^8.67/y - t^3.67*y - t^4.67*y - t^5.*y - t^7.*y - t^7.67*y - 2*t^8.*y - 2*t^8.33*y - t^8.67*y + t^8.33*y^2 + t^8.67*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


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
45081 SO5adj1nf2 $q_1^3q_2$ + $ q_2^2$ + $ \phi_1^2X_1$ + $ q_1^2X_2$ + $ M_1\phi_1^4$ 1.142 1.1489 0.994 [X:[1.5556, 1.3333], M:[1.1111], q:[0.3333, 1.0], qb:[], phi:[0.2222]] t^2.33 + 2*t^3.33 + t^4. + 2*t^4.67 + 2*t^5.67 - t^6. - t^3.67/y - t^4.67/y - t^5./y - t^6./y - t^3.67*y - t^4.67*y - t^5.*y - t^6.*y detail {a: 185/162, c: 1489/1296, X1: 14/9, X2: 4/3, M1: 10/9, q1: 1/3, q2: 1, phi1: 2/9}