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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
45142 SO5adj1nf2 $M_1\phi_1^2q_1$ + $ M_1q_2^2$ + $ M_2q_2^2$ + $ q_1^2q_2^2$ + $ \phi_1^2X_1$ 1.7701 1.8673 0.9479 [X:[1.3333], M:[0.8889, 0.8889], q:[0.4444, 0.5556], qb:[], phi:[0.3333]] [X:[[0]], M:[[0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 1147/648, c: 605/324, X1: 4/3, M1: 8/9, M2: 8/9, q1: 4/9, q2: 5/9, phi1: 1/3}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ M_2$, $ q_1^2$, $ q_1q_2$, $ \phi_1^2q_2$, $ \phi_1^4$, $ \phi_1q_1q_2$, $ X_1$, $ \phi_1^2q_1^2$, $ \phi_1^2q_1q_2$, $ M_1^2$, $ M_1M_2$, $ M_2^2$, $ M_1q_1^2$, $ M_2q_1^2$, $ q_1^4$, $ \phi_1^2q_2^2$, $ M_2q_1q_2$, $ q_1^3q_2$ $\phi_1^3q_1q_2$ 0 3*t^2.67 + t^3. + t^3.67 + 3*t^4. + t^4.67 + t^5. + 7*t^5.33 + 2*t^5.67 + t^6.33 + 8*t^6.67 + 2*t^7. + 3*t^7.33 + 6*t^7.67 + 18*t^8. + 3*t^8.33 - t^4./y - t^5.33/y - t^5.67/y - t^6./y - (3*t^6.67)/y - t^7./y - t^7.67/y - (5*t^8.)/y - t^4.*y - t^5.33*y - t^5.67*y - t^6.*y - 3*t^6.67*y - t^7.*y - t^7.67*y - 5*t^8.*y 3*t^2.67 + t^3. + t^3.67 + 3*t^4. + t^4.67 + t^5. + 7*t^5.33 + 2*t^5.67 + t^6.33 + 8*t^6.67 + 2*t^7. + 3*t^7.33 + 6*t^7.67 + 18*t^8. + 3*t^8.33 - t^4./y - t^5.33/y - t^5.67/y - t^6./y - (3*t^6.67)/y - t^7./y - t^7.67/y - (5*t^8.)/y - t^4.*y - t^5.33*y - t^5.67*y - t^6.*y - 3*t^6.67*y - t^7.*y - t^7.67*y - 5*t^8.*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
45389 $M_1\phi_1^2q_1$ + $ M_1q_2^2$ + $ M_2q_2^2$ + $ q_1^2q_2^2$ + $ \phi_1^2X_1$ + $ M_3\phi_1^2q_2$ 1.7878 1.8989 0.9415 [X:[1.3333], M:[0.8889, 0.8889, 0.7778], q:[0.4444, 0.5556], qb:[], phi:[0.3333]] t^2.33 + 3*t^2.67 + t^3. + 3*t^4. + 2*t^4.67 + 4*t^5. + 8*t^5.33 + 2*t^5.67 - t^4./y - t^5.33/y - t^5.67/y - t^6./y - t^4.*y - t^5.33*y - t^5.67*y - t^6.*y detail {a: 2317/1296, c: 2461/1296, X1: 4/3, M1: 8/9, M2: 8/9, M3: 7/9, q1: 4/9, q2: 5/9, phi1: 1/3}


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