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
46069 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ 0.5288 0.6722 0.7867 [X:[], M:[1.0588], q:[0.7647, 0.1765], qb:[0.5294, 0.6471], phi:[0.4706]] [X:[], M:[[0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 41571/78608, c: 26421/39304, M1: 18/17, q1: 13/17, q2: 3/17, qb1: 9/17, qb2: 11/17, phi1: 8/17}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}^{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ ${}\phi_{1}^{2}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ 2 t^2.12 + 2*t^2.47 + t^2.82 + t^3.18 + 2*t^3.53 + 2*t^3.88 + 2*t^4.24 + 2*t^4.59 + 4*t^4.94 + 4*t^5.29 + 2*t^5.65 + 2*t^6. + 4*t^6.35 + 4*t^6.71 + 4*t^7.06 + 6*t^7.41 + 6*t^7.76 + 4*t^8.12 + 2*t^8.47 + 3*t^8.82 - t^4.41/y + (2*t^7.59)/y + (2*t^7.94)/y + (3*t^8.29)/y + (4*t^8.65)/y - t^4.41*y + 2*t^7.59*y + 2*t^7.94*y + 3*t^8.29*y + 4*t^8.65*y t^2.12 + 2*t^2.47 + t^2.82 + t^3.18 + 2*t^3.53 + 2*t^3.88 + 2*t^4.24 + 2*t^4.59 + 4*t^4.94 + 4*t^5.29 + 2*t^5.65 + 2*t^6. + 4*t^6.35 + 4*t^6.71 + 4*t^7.06 + 6*t^7.41 + 6*t^7.76 + 4*t^8.12 + 2*t^8.47 + 3*t^8.82 - t^4.41/y + (2*t^7.59)/y + (2*t^7.94)/y + (3*t^8.29)/y + (4*t^8.65)/y - t^4.41*y + 2*t^7.59*y + 2*t^7.94*y + 3*t^8.29*y + 4*t^8.65*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
45936 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ 0.5949 0.7584 0.7845 [X:[], M:[0.9671], q:[0.7418, 0.2911], qb:[0.4836, 0.4178], phi:[0.5164]] t^2.13 + t^2.32 + t^2.7 + t^2.9 + t^3.1 + t^3.3 + t^3.48 + 2*t^3.68 + t^3.87 + t^4.06 + 2*t^4.25 + 2*t^4.45 + t^4.65 + t^4.83 + 2*t^5.03 + 2*t^5.23 + t^5.41 + t^5.42 + 2*t^5.61 + 3*t^5.8 + t^6. - t^4.55/y - t^4.55*y detail