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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
45250 SO5adj1nf2 $M_1\phi_1^2q_1$ + $ M_2q_2^2$ + $ M_1q_1^2$ + $ \phi_1^2X_1$ + $ M_3q_1^2$ 1.7362 1.8303 0.9486 [X:[1.398], M:[0.796, 1.0101, 0.796], q:[0.602, 0.495], qb:[], phi:[0.301]] [X:[[2]], M:[[4], [-10], [4]], q:[[-2], [5]], qb:[], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ M_3$, $ M_2$, $ \phi_1^2q_2$, $ q_1q_2$, $ \phi_1^4$, $ \phi_1q_1q_2$, $ X_1$, $ M_1^2$, $ M_1M_3$, $ M_3^2$, $ \phi_1^2q_2^2$, $ \phi_1^2q_1q_2$, $ M_1M_2$, $ M_2M_3$, $ \phi_1^2q_1^2$, $ M_3\phi_1^2q_2$, $ M_1q_1q_2$, $ M_3q_1q_2$ $M_3\phi_1^4$, $ \phi_1^3q_1q_2$ 0 2*t^2.39 + t^3.03 + 2*t^3.29 + t^3.61 + 2*t^4.19 + 4*t^4.78 + t^5.1 + 3*t^5.42 + 3*t^5.68 + t^6.06 + 6*t^6.58 + t^6.64 + t^6.9 + 6*t^7.16 + 2*t^7.22 + 5*t^7.48 + 7*t^7.81 + 6*t^8.07 + 2*t^8.39 + 3*t^8.45 + t^8.71 + 9*t^8.97 - t^3.9/y - t^5.39/y - (2*t^5.71)/y - (2*t^6.29)/y - t^6.93/y - (2*t^7.19)/y - t^7.52/y - t^7.78/y - (4*t^8.1)/y + (2*t^8.42)/y - t^8.68/y - (2*t^8.74)/y - t^3.9*y - t^5.39*y - 2*t^5.71*y - 2*t^6.29*y - t^6.93*y - 2*t^7.19*y - t^7.52*y - t^7.78*y - 4*t^8.1*y + 2*t^8.42*y - t^8.68*y - 2*t^8.74*y 2*g1^4*t^2.39 + t^3.03/g1^10 + 2*g1^3*t^3.29 + t^3.61/g1^4 + 2*g1^2*t^4.19 + 4*g1^8*t^4.78 + g1*t^5.1 + (3*t^5.42)/g1^6 + 3*g1^7*t^5.68 + t^6.06/g1^20 + 6*g1^6*t^6.58 + t^6.64/g1^14 + t^6.9/g1 + 6*g1^12*t^7.16 + (2*t^7.22)/g1^8 + 5*g1^5*t^7.48 + (7*t^7.81)/g1^2 + 6*g1^11*t^8.07 + 2*g1^4*t^8.39 + (3*t^8.45)/g1^16 + t^8.71/g1^3 + 9*g1^10*t^8.97 - t^3.9/(g1*y) - (g1^4*t^5.39)/y - (2*t^5.71)/(g1^3*y) - (2*g1^3*t^6.29)/y - t^6.93/(g1^11*y) - (2*g1^2*t^7.19)/y - t^7.52/(g1^5*y) - (g1^8*t^7.78)/y - (4*g1*t^8.1)/y + (2*t^8.42)/(g1^6*y) - (g1^7*t^8.68)/y - (2*t^8.74)/(g1^13*y) - (t^3.9*y)/g1 - g1^4*t^5.39*y - (2*t^5.71*y)/g1^3 - 2*g1^3*t^6.29*y - (t^6.93*y)/g1^11 - 2*g1^2*t^7.19*y - (t^7.52*y)/g1^5 - g1^8*t^7.78*y - 4*g1*t^8.1*y + (2*t^8.42*y)/g1^6 - g1^7*t^8.68*y - (2*t^8.74*y)/g1^13


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
45036 SO5adj1nf2 $M_1\phi_1^2q_1$ + $ M_2q_2^2$ + $ M_1q_1^2$ + $ \phi_1^2X_1$ 1.7197 1.8009 0.9549 [X:[1.4015], M:[0.803, 0.9925], q:[0.5985, 0.5038], qb:[], phi:[0.2992]] t^2.41 + t^2.98 + 2*t^3.31 + 2*t^3.59 + 2*t^4.2 + 2*t^4.82 + t^5.1 + 2*t^5.39 + t^5.72 + t^5.95 - t^3.9/y - t^5.41/y - (2*t^5.69)/y - t^3.9*y - t^5.41*y - 2*t^5.69*y detail