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
58632 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{3}q_{2}^{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{2}$ + ${ }q_{2}\tilde{q}_{1}X_{3}$ 0.8916 1.0077 0.8848 [X:[1.1429, 1.4286, 1.4286], M:[], q:[1.2381, 0.381], qb:[0.1905, 0.4762], phi:[0.2857]] [X:[[0], [0], [0]], M:[], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 699/784, c: 395/392, X1: 8/7, X2: 10/7, X3: 10/7, q1: 26/21, q2: 8/21, qb1: 4/21, qb2: 10/21, phi1: 2/7}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }X_{2}$, ${ }X_{3}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}\phi_{1}^{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{5}$, ${ }\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{4}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}X_{1}$ 3 2*t^2.57 + 3*t^3.43 + 4*t^4.29 + 3*t^5.14 + 3*t^6. + 8*t^6.86 + 9*t^7.71 + 8*t^8.57 + t^8.57/y^2 - t^3.86/y - t^4.71/y - t^6.43/y - (2*t^7.29)/y - (2*t^8.14)/y - t^3.86*y - t^4.71*y - t^6.43*y - 2*t^7.29*y - 2*t^8.14*y + t^8.57*y^2 2*t^2.57 + 3*t^3.43 + 4*t^4.29 + 3*t^5.14 + 3*t^6. + 8*t^6.86 + 9*t^7.71 + 8*t^8.57 + t^8.57/y^2 - t^3.86/y - t^4.71/y - t^6.43/y - (2*t^7.29)/y - (2*t^8.14)/y - t^3.86*y - t^4.71*y - t^6.43*y - 2*t^7.29*y - 2*t^8.14*y + t^8.57*y^2


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
57589 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{3}q_{2}^{3}$ 1.1809 1.3826 0.8541 [X:[1.4855], M:[], q:[0.8098, 0.2953], qb:[0.4474, 0.2192], phi:[0.3714]] 2*t^2.23 + t^2.66 + t^3.09 + 2*t^3.34 + 3*t^3.77 + t^4.2 + 5*t^4.46 + 4*t^4.89 + 5*t^5.32 + 3*t^5.57 + t^5.74 + 6*t^6. - t^4.11/y - t^5.23/y - t^4.11*y - t^5.23*y detail