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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
8632 Sp2adj1nf1 $\phi_1^2X_1$ + $ M_1q_1q_2$ + $ M_1\phi_1^4$ + $ M_2\phi_1q_1^2$ + $ M_3\phi_1^4$ 1.1226 1.238 0.9068 [X:[1.6], M:[1.2, 0.9546, 1.2], q:[0.4227, 0.3773], qb:[], phi:[0.2]] [X:[[0]], M:[[0], [2], [0]], q:[[-1], [1]], qb:[], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_2$, $ \phi_1q_2^2$, $ \phi_1q_1q_2$, $ M_1$, $ M_3$, $ \phi_1^2q_1q_2$, $ \phi_1^3q_2^2$, $ \phi_1^3q_1q_2$, $ \phi_1^3q_1^2$, $ X_1$, $ M_2^2$, $ M_2\phi_1q_2^2$, $ \phi_1^2q_2^4$, $ M_2\phi_1q_1q_2$, $ \phi_1^2q_1q_2^3$ $\phi_1^2q_1^2q_2^2$ -1 2*t^2.86 + t^3. + 3*t^3.6 + t^4.06 + t^4.2 + t^4.34 + t^4.8 + 3*t^5.73 + t^5.86 - t^6. - t^6.14 + 5*t^6.46 + 2*t^6.6 - t^6.74 + 2*t^6.93 + 2*t^7.06 + 7*t^7.2 + 3*t^7.66 + 2*t^7.8 + t^7.94 + t^8.13 + t^8.26 + 4*t^8.4 + t^8.54 + 4*t^8.59 + t^8.67 + t^8.73 - 3*t^8.86 + t^8.4/y^2 - t^3.6/y - t^4.8/y - (2*t^6.46)/y - t^6.6/y - (2*t^7.2)/y - (2*t^7.66)/y - t^7.8/y - (2*t^8.4)/y + t^8.73/y + (2*t^8.86)/y - t^3.6*y - t^4.8*y - 2*t^6.46*y - t^6.6*y - 2*t^7.2*y - 2*t^7.66*y - t^7.8*y - 2*t^8.4*y + t^8.73*y + 2*t^8.86*y + t^8.4*y^2 2*g1^2*t^2.86 + t^3. + 3*t^3.6 + g1^2*t^4.06 + t^4.2 + t^4.34/g1^2 + t^4.8 + 3*g1^4*t^5.73 + g1^2*t^5.86 - t^6. - t^6.14/g1^2 + 5*g1^2*t^6.46 + 2*t^6.6 - t^6.74/g1^2 + 2*g1^4*t^6.93 + 2*g1^2*t^7.06 + 7*t^7.2 + 3*g1^2*t^7.66 + 2*t^7.8 + t^7.94/g1^2 + g1^4*t^8.13 + g1^2*t^8.26 + 4*t^8.4 + t^8.54/g1^2 + 4*g1^6*t^8.59 + t^8.67/g1^4 + g1^4*t^8.73 - 3*g1^2*t^8.86 + t^8.4/y^2 - t^3.6/y - t^4.8/y - (2*g1^2*t^6.46)/y - t^6.6/y - (2*t^7.2)/y - (2*g1^2*t^7.66)/y - t^7.8/y - (2*t^8.4)/y + (g1^4*t^8.73)/y + (2*g1^2*t^8.86)/y - t^3.6*y - t^4.8*y - 2*g1^2*t^6.46*y - t^6.6*y - 2*t^7.2*y - 2*g1^2*t^7.66*y - t^7.8*y - 2*t^8.4*y + g1^4*t^8.73*y + 2*g1^2*t^8.86*y + t^8.4*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
8470 Sp2adj1nf1 $\phi_1^2X_1$ + $ M_1q_1q_2$ + $ M_1\phi_1^4$ + $ M_2\phi_1q_1^2$ 1.1391 1.267 0.8991 [X:[1.6], M:[1.2, 0.9546], q:[0.4227, 0.3773], qb:[], phi:[0.2]] t^2.4 + 2*t^2.86 + t^3. + 2*t^3.6 + t^4.06 + t^4.2 + t^4.34 + 2*t^4.8 + 2*t^5.26 + t^5.4 + 3*t^5.73 + t^5.86 + t^6. - t^3.6/y - t^4.8/y - t^6./y - t^3.6*y - t^4.8*y - t^6.*y detail