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
46166 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{1}$ 0.4904 0.6206 0.7902 [X:[1.5917], M:[0.4083, 1.1834, 0.7751], q:[0.4083, 1.1834], qb:[0.4083, 0.3667], phi:[0.4083]] [X:[[1]], M:[[-1], [2], [3]], q:[[-1], [2]], qb:[[-1], [4]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$, ${ }M_{2}M_{3}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ ${}M_{3}\phi_{1}q_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{3}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$ -3 3*t^2.325 + t^2.45 + t^3.425 + 2*t^3.55 + 7*t^4.65 + 4*t^4.775 + 3*t^5.751 + 5*t^5.875 - 3*t^6. - 2*t^6.125 + t^6.851 + 14*t^6.975 + 7*t^7.1 - 4*t^7.225 - t^7.35 + 7*t^8.076 + 10*t^8.2 - 11*t^8.325 - 8*t^8.45 - t^8.575 - t^4.225/y - t^6.55/y + (3*t^7.65)/y + (3*t^7.775)/y + t^7.9/y + (3*t^8.751)/y + (6*t^8.875)/y - t^4.225*y - t^6.55*y + 3*t^7.65*y + 3*t^7.775*y + t^7.9*y + 3*t^8.751*y + 6*t^8.875*y 3*g1^3*t^2.325 + t^2.45/g1^2 + g1^7*t^3.425 + 2*g1^2*t^3.55 + 7*g1^6*t^4.65 + 4*g1*t^4.775 + 3*g1^10*t^5.751 + 5*g1^5*t^5.875 - 3*t^6. - (2*t^6.125)/g1^5 + g1^14*t^6.851 + 14*g1^9*t^6.975 + 7*g1^4*t^7.1 - (4*t^7.225)/g1 - t^7.35/g1^6 + 7*g1^13*t^8.076 + 10*g1^8*t^8.2 - 11*g1^3*t^8.325 - (8*t^8.45)/g1^2 - t^8.575/g1^7 - t^4.225/(g1*y) - (g1^2*t^6.55)/y + (3*g1^6*t^7.65)/y + (3*g1*t^7.775)/y + t^7.9/(g1^4*y) + (3*g1^10*t^8.751)/y + (6*g1^5*t^8.875)/y - (t^4.225*y)/g1 - g1^2*t^6.55*y + 3*g1^6*t^7.65*y + 3*g1*t^7.775*y + (t^7.9*y)/g1^4 + 3*g1^10*t^8.751*y + 6*g1^5*t^8.875*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
46034 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ 0.4728 0.5871 0.8053 [X:[1.5958], M:[0.4042, 1.1917], q:[0.4042, 1.1917], qb:[0.4042, 0.3833], phi:[0.4042]] 2*t^2.362 + t^2.425 + t^3.512 + 2*t^3.575 + t^3.638 + 4*t^4.725 + 3*t^4.787 + 2*t^5.875 + 3*t^5.937 - t^6. - t^4.213/y - t^4.213*y detail