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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
45565 SO5adj1nf2 $M_1\phi_1^2q_1$ + $ q_1^3q_2$ + $ M_1q_2^2$ + $ \phi_1^2X_1$ + $ M_2q_2^2$ + $ M_3\phi_1^2q_2$ + $ M_4\phi_1^4$ + $ M_5q_1q_2$ 1.8018 1.9268 0.9351 [X:[1.36], M:[0.88, 0.88, 0.8, 0.72, 0.96], q:[0.48, 0.56], qb:[], phi:[0.32]] [X:[[0]], M:[[0], [0], [0], [0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 225231/125000, c: 30107/15625, X1: 34/25, M1: 22/25, M2: 22/25, M3: 4/5, M4: 18/25, M5: 24/25, q1: 12/25, q2: 14/25, phi1: 8/25}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_4$, $ M_3$, $ M_1$, $ M_2$, $ M_5$, $ q_1^2$, $ \phi_1q_1q_2$, $ X_1$, $ M_4^2$, $ M_3M_4$, $ M_3^2$, $ M_1M_4$, $ M_2M_4$, $ \phi_1^2q_1^2$, $ M_1M_3$, $ M_2M_3$, $ M_4M_5$, $ M_4q_1^2$, $ \phi_1^2q_1q_2$, $ M_1^2$, $ M_1M_2$, $ M_2^2$, $ M_3M_5$, $ M_3q_1^2$, $ \phi_1^2q_2^2$, $ M_1M_5$, $ M_2M_5$, $ M_1q_1^2$, $ M_2q_1^2$, $ M_5^2$, $ M_5q_1^2$ $\phi_1^3q_1q_2$ -1 t^2.16 + t^2.4 + 2*t^2.64 + 2*t^2.88 + 2*t^4.08 + t^4.32 + t^4.56 + 4*t^4.8 + 5*t^5.04 + 6*t^5.28 + 4*t^5.52 + 2*t^5.76 - t^6. + 2*t^6.48 + 4*t^6.72 + 7*t^6.96 + 6*t^7.2 + 11*t^7.44 + 13*t^7.68 + 13*t^7.92 + 10*t^8.16 + 2*t^8.4 - 2*t^8.64 - t^3.96/y - t^5.4/y - t^5.64/y - t^5.88/y - t^6.12/y - t^6.36/y - (2*t^6.6)/y - (2*t^6.84)/y - t^8.04/y - (2*t^8.28)/y - (4*t^8.76)/y - t^3.96*y - t^5.4*y - t^5.64*y - t^5.88*y - t^6.12*y - t^6.36*y - 2*t^6.6*y - 2*t^6.84*y - t^8.04*y - 2*t^8.28*y - 4*t^8.76*y t^2.16 + t^2.4 + 2*t^2.64 + 2*t^2.88 + 2*t^4.08 + t^4.32 + t^4.56 + 4*t^4.8 + 5*t^5.04 + 6*t^5.28 + 4*t^5.52 + 2*t^5.76 - t^6. + 2*t^6.48 + 4*t^6.72 + 7*t^6.96 + 6*t^7.2 + 11*t^7.44 + 13*t^7.68 + 13*t^7.92 + 10*t^8.16 + 2*t^8.4 - 2*t^8.64 - t^3.96/y - t^5.4/y - t^5.64/y - t^5.88/y - t^6.12/y - t^6.36/y - (2*t^6.6)/y - (2*t^6.84)/y - t^8.04/y - (2*t^8.28)/y - (4*t^8.76)/y - t^3.96*y - t^5.4*y - t^5.64*y - t^5.88*y - t^6.12*y - t^6.36*y - 2*t^6.6*y - 2*t^6.84*y - t^8.04*y - 2*t^8.28*y - 4*t^8.76*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


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
45460 SO5adj1nf2 $M_1\phi_1^2q_1$ + $ q_1^3q_2$ + $ M_1q_2^2$ + $ \phi_1^2X_1$ + $ M_2q_2^2$ + $ M_3\phi_1^2q_2$ + $ M_4\phi_1^4$ 1.7981 1.9206 0.9362 [X:[1.36], M:[0.88, 0.88, 0.8, 0.72], q:[0.48, 0.56], qb:[], phi:[0.32]] t^2.16 + t^2.4 + 2*t^2.64 + t^2.88 + t^3.12 + 2*t^4.08 + t^4.32 + t^4.56 + 4*t^4.8 + 4*t^5.04 + 6*t^5.28 + 3*t^5.52 + 2*t^5.76 - t^3.96/y - t^5.4/y - t^5.64/y - t^5.88/y - t^3.96*y - t^5.4*y - t^5.64*y - t^5.88*y detail {a: 449529/250000, c: 240077/125000, X1: 34/25, M1: 22/25, M2: 22/25, M3: 4/5, M4: 18/25, q1: 12/25, q2: 14/25, phi1: 8/25}