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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
45231 SO5adj1nf2 $q_1^3q_2$ + $ M_1q_1q_2$ + $ \phi_1^2q_2^2$ + $ \phi_1^2X_1$ + $ M_2\phi_1^4$ 1.6334 1.7137 0.9531 [X:[1.4286], M:[0.8571, 0.8571], q:[0.4286, 0.7143], qb:[], phi:[0.2857]] [X:[[0]], M:[[0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 2241/1372, c: 9405/5488, X1: 10/7, M1: 6/7, M2: 6/7, q1: 3/7, q2: 5/7, phi1: 2/7}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ M_2$, $ q_1^2$, $ \phi_1^2q_1$, $ \phi_1^2q_2$, $ \phi_1^2q_1^2$, $ \phi_1q_1q_2$, $ q_2^2$, $ X_1$, $ M_1^2$, $ M_1M_2$, $ M_2^2$, $ M_1q_1^2$, $ M_2q_1^2$, $ \phi_1^2q_1q_2$, $ M_1\phi_1^2q_1$, $ M_2\phi_1^2q_1$ $\phi_1^4q_1^2$, $ \phi_1^3q_1q_2$ 0 3*t^2.57 + t^3. + t^3.86 + 4*t^4.29 + 6*t^5.14 + 2*t^5.57 + 2*t^6.43 + 10*t^6.86 + 4*t^7.29 + 8*t^7.71 + 6*t^8.14 + 7*t^8.57 - t^3.86/y - t^5.14/y - t^5.57/y - t^6./y - (3*t^6.43)/y - t^6.86/y - (3*t^7.71)/y - (3*t^8.14)/y + t^8.57/y - t^3.86*y - t^5.14*y - t^5.57*y - t^6.*y - 3*t^6.43*y - t^6.86*y - 3*t^7.71*y - 3*t^8.14*y + t^8.57*y 3*t^2.57 + t^3. + t^3.86 + 4*t^4.29 + 6*t^5.14 + 2*t^5.57 + 2*t^6.43 + 10*t^6.86 + 4*t^7.29 + 8*t^7.71 + 6*t^8.14 + 7*t^8.57 - t^3.86/y - t^5.14/y - t^5.57/y - t^6./y - (3*t^6.43)/y - t^6.86/y - (3*t^7.71)/y - (3*t^8.14)/y + t^8.57/y - t^3.86*y - t^5.14*y - t^5.57*y - t^6.*y - 3*t^6.43*y - t^6.86*y - 3*t^7.71*y - 3*t^8.14*y + t^8.57*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
45390 $q_1^3q_2$ + $ M_1q_1q_2$ + $ \phi_1^2q_2^2$ + $ \phi_1^2X_1$ + $ M_2\phi_1^4$ + $ M_3\phi_1^2q_2$ 1.6536 1.7518 0.9439 [X:[1.4286], M:[0.8571, 0.8571, 0.7143], q:[0.4286, 0.7143], qb:[], phi:[0.2857]] t^2.14 + 3*t^2.57 + t^3. + 5*t^4.29 + 3*t^4.71 + 7*t^5.14 + 2*t^5.57 - t^3.86/y - t^5.14/y - t^5.57/y - (2*t^6.)/y - t^3.86*y - t^5.14*y - t^5.57*y - 2*t^6.*y detail {a: 9075/5488, c: 4807/2744, X1: 10/7, M1: 6/7, M2: 6/7, M3: 5/7, q1: 3/7, q2: 5/7, phi1: 2/7}


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
45091 SO5adj1nf2 $q_1^3q_2$ + $ M_1q_1q_2$ + $ \phi_1^2q_2^2$ + $ \phi_1^2X_1$ 1.6208 1.6922 0.9578 [X:[1.4286], M:[0.8571], q:[0.4286, 0.7143], qb:[], phi:[0.2857]] 2*t^2.57 + t^3. + t^3.43 + t^3.86 + 4*t^4.29 + 3*t^5.14 + t^5.57 + 2*t^6. - t^3.86/y - t^5.14/y - t^5.57/y - t^6./y - t^3.86*y - t^5.14*y - t^5.57*y - t^6.*y detail {a: 8895/5488, c: 9287/5488, X1: 10/7, M1: 6/7, q1: 3/7, q2: 5/7, phi1: 2/7}