Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

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
56462 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{5}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{4}M_{7}$ 0.7183 0.89 0.807 [M:[0.9449, 0.8347, 0.9449, 1.0551, 1.0551, 0.8347, 0.9449], q:[0.5275, 0.5275], qb:[0.6377, 0.4174], phi:[0.4725]] [M:[[2], [6], [2], [-2], [-2], [6], [2]], q:[[-1], [-1]], qb:[[-5], [3]], phi:[[1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{3}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$ ${}M_{1}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$ -2 2*t^2.504 + 4*t^2.835 + t^3.165 + t^3.922 + 2*t^4.252 + 4*t^4.583 + 2*t^4.913 + 3*t^5.008 + t^5.244 + 7*t^5.339 + 8*t^5.669 - 2*t^6. - 4*t^6.331 + 2*t^6.426 - t^6.661 + 7*t^6.756 + 11*t^7.087 + 11*t^7.417 + 4*t^7.513 + t^7.748 + 11*t^7.843 - t^8.078 + 14*t^8.174 - t^8.409 + 6*t^8.504 - 14*t^8.835 + 3*t^8.93 - t^4.417/y - (2*t^6.922)/y - (2*t^7.252)/y + (2*t^7.583)/y + (2*t^7.913)/y + t^8.008/y + (8*t^8.339)/y + (8*t^8.669)/y - t^4.417*y - 2*t^6.922*y - 2*t^7.252*y + 2*t^7.583*y + 2*t^7.913*y + t^8.008*y + 8*t^8.339*y + 8*t^8.669*y 2*g1^6*t^2.504 + 4*g1^2*t^2.835 + t^3.165/g1^2 + g1^7*t^3.922 + 2*g1^3*t^4.252 + (4*t^4.583)/g1 + (2*t^4.913)/g1^5 + 3*g1^12*t^5.008 + t^5.244/g1^9 + 7*g1^8*t^5.339 + 8*g1^4*t^5.669 - 2*t^6. - (4*t^6.331)/g1^4 + 2*g1^13*t^6.426 - t^6.661/g1^8 + 7*g1^9*t^6.756 + 11*g1^5*t^7.087 + 11*g1*t^7.417 + 4*g1^18*t^7.513 + t^7.748/g1^3 + 11*g1^14*t^7.843 - t^8.078/g1^7 + 14*g1^10*t^8.174 - t^8.409/g1^11 + 6*g1^6*t^8.504 - 14*g1^2*t^8.835 + 3*g1^19*t^8.93 - (g1*t^4.417)/y - (2*g1^7*t^6.922)/y - (2*g1^3*t^7.252)/y + (2*t^7.583)/(g1*y) + (2*t^7.913)/(g1^5*y) + (g1^12*t^8.008)/y + (8*g1^8*t^8.339)/y + (8*g1^4*t^8.669)/y - g1*t^4.417*y - 2*g1^7*t^6.922*y - 2*g1^3*t^7.252*y + (2*t^7.583*y)/g1 + (2*t^7.913*y)/g1^5 + g1^12*t^8.008*y + 8*g1^8*t^8.339*y + 8*g1^4*t^8.669*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
53488 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{5}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{1}M_{4}$ 0.7134 0.8806 0.8101 [M:[0.9499, 0.8496, 0.9499, 1.0501, 1.0501, 0.8496], q:[0.5251, 0.5251], qb:[0.6253, 0.4248], phi:[0.4749]] 2*t^2.549 + 3*t^2.85 + 2*t^3.15 + t^3.974 + 2*t^4.274 + 4*t^4.575 + 2*t^4.876 + 3*t^5.098 + t^5.177 + 5*t^5.398 + 6*t^5.699 - t^4.425/y - t^4.425*y detail