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
59436 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{2}$ + ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ 1.1991 1.3809 0.8683 [X:[1.2727, 1.4545], M:[], q:[0.7273, 0.1818], qb:[0.5455, 0.3636], phi:[0.3636]] [X:[[0], [0]], M:[], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 1596/1331, c: 1838/1331, X1: 14/11, X2: 16/11, q1: 8/11, q2: 2/11, qb1: 6/11, qb2: 4/11, phi1: 4/11}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$ ${}\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ 2}\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}X_{1}$ 5 t^2.18 + t^2.73 + 3*t^3.27 + 3*t^3.82 + 4*t^4.36 + 4*t^4.91 + 5*t^5.45 + 5*t^6. + 10*t^6.55 + 11*t^7.09 + 14*t^7.64 + 15*t^8.18 + 16*t^8.73 - t^4.09/y - t^5.18/y - t^6.27/y - (3*t^7.36)/y - t^7.91/y - t^8.45/y - t^4.09*y - t^5.18*y - t^6.27*y - 3*t^7.36*y - t^7.91*y - t^8.45*y t^2.18 + t^2.73 + 3*t^3.27 + 3*t^3.82 + 4*t^4.36 + 4*t^4.91 + 5*t^5.45 + 5*t^6. + 10*t^6.55 + 11*t^7.09 + 14*t^7.64 + 15*t^8.18 + 16*t^8.73 - t^4.09/y - t^5.18/y - t^6.27/y - (3*t^7.36)/y - t^7.91/y - t^8.45/y - t^4.09*y - t^5.18*y - t^6.27*y - 3*t^7.36*y - t^7.91*y - t^8.45*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
57711 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{2}$ 1.2026 1.3877 0.8666 [X:[1.2594, 1.4812], M:[], q:[0.7161, 0.1974], qb:[0.5432, 0.3214], phi:[0.3703]] t^2.22 + t^2.67 + t^3.11 + 2*t^3.33 + 3*t^3.78 + t^4.22 + 3*t^4.44 + t^4.67 + 2*t^4.89 + t^5.11 + 3*t^5.33 + 2*t^5.55 + 2*t^5.78 + 3*t^6. - t^4.11/y - t^5.22/y - t^4.11*y - t^5.22*y detail