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
58404 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$ 1.3245 1.5834 0.8365 [X:[], M:[0.8573], q:[0.4951, 0.5524], qb:[0.2476, 0.3049], phi:[0.4]] [X:[], M:[[3]], q:[[-2], [1]], qb:[[-1], [2]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$ ${2}\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ 2}\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ 2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ 2}\phi_{1}^{3}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ 2}\phi_{1}q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ 11 t^2.23 + 3*t^2.4 + 2*t^2.57 + 4*t^3.6 + 2*t^3.77 + t^4.46 + 4*t^4.63 + 11*t^4.8 + 8*t^4.97 + 3*t^5.14 + 4*t^5.83 + 11*t^6. + 12*t^6.17 + 5*t^6.34 + t^6.68 + 4*t^6.86 + 11*t^7.03 + 29*t^7.2 + 27*t^7.37 + 15*t^7.54 + 4*t^7.72 + 5*t^8.06 + 9*t^8.23 + 28*t^8.4 + 33*t^8.57 + 24*t^8.74 + t^8.91 + 8*t^8.92 - t^4.2/y - t^5.4/y - t^6.43/y - (3*t^6.6)/y - (2*t^6.77)/y + (3*t^7.63)/y + (2*t^7.8)/y + (4*t^7.97)/y + t^8.14/y - t^8.66/y + t^8.83/y - t^4.2*y - t^5.4*y - t^6.43*y - 3*t^6.6*y - 2*t^6.77*y + 3*t^7.63*y + 2*t^7.8*y + 4*t^7.97*y + t^8.14*y - t^8.66*y + t^8.83*y t^2.23/g1^3 + 3*t^2.4 + 2*g1^3*t^2.57 + 4*t^3.6 + 2*g1^3*t^3.77 + t^4.46/g1^6 + (4*t^4.63)/g1^3 + 11*t^4.8 + 8*g1^3*t^4.97 + 3*g1^6*t^5.14 + (4*t^5.83)/g1^3 + 11*t^6. + 12*g1^3*t^6.17 + 5*g1^6*t^6.34 + t^6.68/g1^9 + (4*t^6.86)/g1^6 + (11*t^7.03)/g1^3 + 29*t^7.2 + 27*g1^3*t^7.37 + 15*g1^6*t^7.54 + 4*g1^9*t^7.72 + (5*t^8.06)/g1^6 + (9*t^8.23)/g1^3 + 28*t^8.4 + 33*g1^3*t^8.57 + 24*g1^6*t^8.74 + t^8.91/g1^12 + 8*g1^9*t^8.92 - t^4.2/y - t^5.4/y - t^6.43/(g1^3*y) - (3*t^6.6)/y - (2*g1^3*t^6.77)/y + (3*t^7.63)/(g1^3*y) + (2*t^7.8)/y + (4*g1^3*t^7.97)/y + (g1^6*t^8.14)/y - t^8.66/(g1^6*y) + t^8.83/(g1^3*y) - t^4.2*y - t^5.4*y - (t^6.43*y)/g1^3 - 3*t^6.6*y - 2*g1^3*t^6.77*y + (3*t^7.63*y)/g1^3 + 2*t^7.8*y + 4*g1^3*t^7.97*y + g1^6*t^8.14*y - (t^8.66*y)/g1^6 + (t^8.83*y)/g1^3


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
57344 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ 1.3363 1.595 0.8378 [M:[0.8611], q:[0.4375, 0.5812], qb:[0.3014, 0.2798], phi:[0.4]] t^2.152 + t^2.217 + t^2.4 + 2*t^2.583 + t^2.648 + t^3.352 + t^3.6 + 2*t^3.783 + 2*t^3.848 + t^4.304 + t^4.369 + t^4.434 + 2*t^4.552 + 2*t^4.617 + 2*t^4.735 + 4*t^4.8 + t^4.865 + 4*t^4.983 + 3*t^5.048 + 3*t^5.166 + 2*t^5.231 + t^5.296 + t^5.504 + t^5.569 + 2*t^5.752 + t^5.817 + 3*t^5.935 + 2*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail