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
61129 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ + ${ }q_{2}\tilde{q}_{1}X_{1}$ 1.3242 1.5527 0.8528 [X:[1.4], M:[0.772, 1.172], q:[0.552, 0.324], qb:[0.276, 0.448], phi:[0.4]] [X:[[0]], M:[[3], [3]], q:[[-2], [1]], qb:[[-1], [2]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ 1 2*t^2.32 + t^2.4 + 2*t^3. + 2*t^3.52 + t^3.6 + 4*t^4.2 + 3*t^4.63 + 4*t^4.72 + 2*t^4.8 + t^4.88 + 3*t^5.32 + 4*t^5.4 + 4*t^5.83 + 5*t^5.92 + t^6. + t^6.08 + 10*t^6.52 + 6*t^6.6 - t^6.68 + 4*t^6.95 + 10*t^7.03 + 8*t^7.12 + 8*t^7.2 - t^7.28 + 5*t^7.63 + 14*t^7.72 + 5*t^7.8 + 6*t^8.15 + 12*t^8.23 + 4*t^8.32 + 11*t^8.4 - 3*t^8.48 + t^8.57 + 14*t^8.83 + 20*t^8.92 - t^4.2/y - t^5.4/y - (2*t^6.52)/y - t^6.6/y - t^7.2/y + t^7.63/y - t^7.72/y - t^7.8/y + t^7.88/y + (4*t^8.32)/y - t^8.4/y + t^8.83/y - t^4.2*y - t^5.4*y - 2*t^6.52*y - t^6.6*y - t^7.2*y + t^7.63*y - t^7.72*y - t^7.8*y + t^7.88*y + 4*t^8.32*y - t^8.4*y + t^8.83*y 2*g1^3*t^2.32 + t^2.4 + 2*t^3. + 2*g1^3*t^3.52 + t^3.6 + 4*t^4.2 + 3*g1^6*t^4.63 + 4*g1^3*t^4.72 + 2*t^4.8 + t^4.88/g1^3 + 3*g1^3*t^5.32 + 4*t^5.4 + 4*g1^6*t^5.83 + 5*g1^3*t^5.92 + t^6. + t^6.08/g1^3 + 10*g1^3*t^6.52 + 6*t^6.6 - t^6.68/g1^3 + 4*g1^9*t^6.95 + 10*g1^6*t^7.03 + 8*g1^3*t^7.12 + 8*t^7.2 - t^7.28/g1^3 + 5*g1^6*t^7.63 + 14*g1^3*t^7.72 + 5*t^7.8 + 6*g1^9*t^8.15 + 12*g1^6*t^8.23 + 4*g1^3*t^8.32 + 11*t^8.4 - (3*t^8.48)/g1^3 + t^8.57/g1^6 + 14*g1^6*t^8.83 + 20*g1^3*t^8.92 - t^4.2/y - t^5.4/y - (2*g1^3*t^6.52)/y - t^6.6/y - t^7.2/y + (g1^6*t^7.63)/y - (g1^3*t^7.72)/y - t^7.8/y + t^7.88/(g1^3*y) + (4*g1^3*t^8.32)/y - t^8.4/y + (g1^6*t^8.83)/y - t^4.2*y - t^5.4*y - 2*g1^3*t^6.52*y - t^6.6*y - t^7.2*y + g1^6*t^7.63*y - g1^3*t^7.72*y - t^7.8*y + (t^7.88*y)/g1^3 + 4*g1^3*t^8.32*y - t^8.4*y + g1^6*t^8.83*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
58370 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ 1.4121 1.6665 0.8473 [X:[], M:[0.7648, 1.1648], q:[0.4213, 0.3894], qb:[0.4139, 0.3754], phi:[0.4]] 2*t^2.29 + t^2.39 + t^2.4 + t^2.41 + 2*t^3.49 + t^3.59 + t^3.6 + t^3.61 + 3*t^4.59 + 2*t^4.68 + 4*t^4.69 + 2*t^4.7 + t^4.78 + 2*t^4.79 + 3*t^4.8 + 3*t^4.81 + t^4.82 + t^4.9 + t^4.91 + 4*t^5.79 + 3*t^5.88 + 5*t^5.89 + 3*t^5.9 + t^5.98 + 2*t^5.99 - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail