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
199 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}X_{1}$ 0.4728 0.5871 0.8053 [X:[1.5958], M:[1.1917, 0.4042], q:[0.6167, 0.9791], qb:[0.1917, 0.5958], phi:[0.4042]] [X:[[1]], M:[[2], [-1]], q:[[-4], [5]], qb:[[2], [1]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{4}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ ${}\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$ -1 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^6.063 + t^7.025 + 7*t^7.087 + 4*t^7.15 - 2*t^7.213 + 4*t^8.237 + 5*t^8.3 - 4*t^8.362 - 3*t^8.425 - t^8.488 - t^4.213/y + t^7.725/y + (2*t^7.787)/y + (2*t^8.875)/y + (5*t^8.937)/y - t^4.213*y + t^7.725*y + 2*t^7.787*y + 2*t^8.875*y + 5*t^8.937*y 2*g1^3*t^2.362 + t^2.425/g1^2 + g1^7*t^3.512 + 2*g1^2*t^3.575 + t^3.638/g1^3 + 4*g1^6*t^4.725 + 3*g1*t^4.787 + 2*g1^10*t^5.875 + 3*g1^5*t^5.937 - t^6. - t^6.063/g1^5 + g1^14*t^7.025 + 7*g1^9*t^7.087 + 4*g1^4*t^7.15 - (2*t^7.213)/g1 + 4*g1^13*t^8.237 + 5*g1^8*t^8.3 - 4*g1^3*t^8.362 - (3*t^8.425)/g1^2 - t^8.488/g1^7 - t^4.213/(g1*y) + (g1^6*t^7.725)/y + (2*g1*t^7.787)/y + (2*g1^10*t^8.875)/y + (5*g1^5*t^8.937)/y - (t^4.213*y)/g1 + g1^6*t^7.725*y + 2*g1*t^7.787*y + 2*g1^10*t^8.875*y + 5*g1^5*t^8.937*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
121 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ 0.5427 0.6891 0.7875 [M:[1.1204, 0.7357], q:[0.6112, 0.949], qb:[0.2684, 0.4122], phi:[0.4398]] t^2.042 + t^2.207 + t^2.639 + t^2.93 + t^3.07 + 2*t^3.361 + t^3.652 + 2*t^4.084 + t^4.249 + t^4.414 + 2*t^4.681 + t^4.846 + t^4.971 + t^5.112 + t^5.137 + t^5.278 + 2*t^5.403 + 2*t^5.568 + t^5.694 + 2*t^5.859 - t^6. - t^4.319/y - t^4.319*y detail