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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
8207 Sp2adj1nf1 $\phi_1^2X_1$ + $ q_1^2q_2^2$ + $ \phi_1^4X_2$ + $ M_1\phi_1q_1q_2$ 1.1367 1.2305 0.9238 [X:[1.6667, 1.3333], M:[0.8333], q:[0.5, 0.5], qb:[], phi:[0.1667]] [X:[[0], [0]], M:[[0]], q:[[-1], [1]], qb:[], phi:[[0]]] 1 {a: 291/256, c: 315/256, X1: 5/3, X2: 4/3, M1: 5/6, q1: 1/2, q2: 1/2, phi1: 1/6}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ q_1q_2$, $ \phi_1q_1^2$, $ \phi_1q_2^2$, $ \phi_1^2q_1q_2$, $ X_2$, $ \phi_1^3q_1^2$, $ \phi_1^3q_1q_2$, $ \phi_1^3q_2^2$, $ \phi_1^3q_1^2$, $ \phi_1^3q_2^2$, $ M_1^2$, $ X_1$, $ M_1q_1q_2$ $M_1\phi_1q_1^2$, $ M_1\phi_1q_2^2$ -1 t^2.5 + t^3. + 2*t^3.5 + 2*t^4. + 3*t^4.5 + 2*t^5. + t^5.5 - t^6. + t^6.5 + 5*t^7. + 6*t^7.5 + 11*t^8. + 5*t^8.5 + t^8./y^2 - t^3.5/y - t^4.5/y - t^6./y - t^6.5/y - (3*t^7.)/y - (2*t^7.5)/y - (2*t^8.)/y - t^8.5/y - t^3.5*y - t^4.5*y - t^6.*y - t^6.5*y - 3*t^7.*y - 2*t^7.5*y - 2*t^8.*y - t^8.5*y + t^8.*y^2 t^2.5 + t^3. + t^3.5/g1^2 + g1^2*t^3.5 + 2*t^4. + t^4.5 + t^4.5/g1^2 + g1^2*t^4.5 + 2*t^5. + t^5.5 - t^6. + t^6.5 + 3*t^7. + t^7./g1^4 + g1^4*t^7. + 2*t^7.5 + (2*t^7.5)/g1^2 + 2*g1^2*t^7.5 + 7*t^8. + t^8./g1^4 + t^8./g1^2 + g1^2*t^8. + g1^4*t^8. + t^8.5 + (2*t^8.5)/g1^2 + 2*g1^2*t^8.5 + t^8./y^2 - t^3.5/y - t^4.5/y - t^6./y - t^6.5/y - t^7./y - t^7./(g1^2*y) - (g1^2*t^7.)/y - (2*t^7.5)/y - t^8./(g1^2*y) - (g1^2*t^8.)/y - t^8.5/y - t^3.5*y - t^4.5*y - t^6.*y - t^6.5*y - t^7.*y - (t^7.*y)/g1^2 - g1^2*t^7.*y - 2*t^7.5*y - (t^8.*y)/g1^2 - g1^2*t^8.*y - t^8.5*y + t^8.*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
8497 $\phi_1^2X_1$ + $ q_1^2q_2^2$ + $ \phi_1^4X_2$ + $ M_1\phi_1q_1q_2$ + $ \phi_1^3q_1^2$ + $ \phi_1q_2^2X_3$ 0.9049 0.9779 0.9254 [X:[1.6667, 1.3333, 1.3333], M:[0.8333], q:[0.75, 0.25], qb:[], phi:[0.1667]] t^2.5 + 2*t^3. + 3*t^4. + 2*t^5. + t^5.5 + t^6. - t^3.5/y - t^4.5/y - t^6./y - t^3.5*y - t^4.5*y - t^6.*y detail {a: 695/768, c: 751/768, X1: 5/3, X2: 4/3, X3: 4/3, M1: 5/6, q1: 3/4, q2: 1/4, phi1: 1/6}


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
8186 Sp2adj1nf1 $\phi_1^2X_1$ + $ q_1^2q_2^2$ + $ \phi_1^4X_2$ 1.1224 1.2057 0.9309 [X:[1.6667, 1.3333], M:[], q:[0.5, 0.5], qb:[], phi:[0.1667]] t^3. + 3*t^3.5 + 2*t^4. + 3*t^4.5 + t^5. - 3*t^6. - t^3.5/y - t^4.5/y - t^3.5*y - t^4.5*y detail {a: 431/384, c: 463/384, X1: 5/3, X2: 4/3, q1: 1/2, q2: 1/2, phi1: 1/6}