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
113 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ + ${ }M_{1}^{2}$ 0.57 0.6943 0.8211 [M:[1.0], q:[0.5963, 1.0062], qb:[0.4037, 0.4037], phi:[0.3975]] [M:[[0]], q:[[-3], [5]], qb:[[3], [3]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ 1 t^2.385 + t^2.422 + 2*t^3. + 3*t^3.615 + 2*t^4.23 + t^4.77 + 2*t^4.807 + t^4.845 + 2*t^5.422 + t^6. + 3*t^6.037 - 2*t^6.578 + 4*t^6.615 + 2*t^6.652 + t^7.155 - 2*t^7.193 + 7*t^7.23 + t^7.267 - 2*t^7.807 + 6*t^7.845 - 2*t^8.385 + 6*t^8.46 - t^4.193/y - t^6.578/y + (2*t^7.807)/y + (2*t^8.385)/y + (2*t^8.422)/y - t^8.963/y - t^4.193*y - t^6.578*y + 2*t^7.807*y + 2*t^8.385*y + 2*t^8.422*y - t^8.963*y t^2.385/g1^4 + g1^6*t^2.422 + 2*t^3. + 3*g1^4*t^3.615 + 2*g1^8*t^4.23 + t^4.77/g1^8 + 2*g1^2*t^4.807 + g1^12*t^4.845 + 2*g1^6*t^5.422 + t^6. + 3*g1^10*t^6.037 - (2*t^6.578)/g1^6 + 4*g1^4*t^6.615 + 2*g1^14*t^6.652 + t^7.155/g1^12 - (2*t^7.193)/g1^2 + 7*g1^8*t^7.23 + g1^18*t^7.267 - 2*g1^2*t^7.807 + 6*g1^12*t^7.845 - (2*t^8.385)/g1^4 + 6*g1^16*t^8.46 - t^4.193/(g1^2*y) - t^6.578/(g1^6*y) + (2*g1^2*t^7.807)/y + (2*t^8.385)/(g1^4*y) + (2*g1^6*t^8.422)/y - t^8.963/(g1^10*y) - (t^4.193*y)/g1^2 - (t^6.578*y)/g1^6 + 2*g1^2*t^7.807*y + (2*t^8.385*y)/g1^4 + 2*g1^6*t^8.422*y - (t^8.963*y)/g1^10


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
75 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ 0.6281 0.758 0.8286 [M:[0.6967], q:[0.8359, 0.809], qb:[0.4674, 0.4674], phi:[0.3551]] t^2.09 + t^2.13 + t^2.805 + 2*t^3.829 + 3*t^3.87 + t^3.91 + t^4.18 + t^4.22 + t^4.261 + t^4.895 + 2*t^4.935 + t^5.609 + 2*t^5.919 + 3*t^5.96 - t^6. - t^4.065/y - t^4.065*y detail