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
47108 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ 0.6539 0.8186 0.7988 [M:[0.8471, 1.2118, 0.7882, 0.7294, 0.9059], q:[0.7294, 0.4235], qb:[0.3647, 0.7882], phi:[0.4235]] [M:[[-4], [-1], [1], [6], [-9]], q:[[6], [-2]], qb:[[3], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{3}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{4}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ ${}M_{3}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ 2 t^2.188 + t^2.365 + 2*t^2.541 + t^2.718 + 2*t^3.459 + 2*t^3.635 + t^4.376 + 3*t^4.553 + 4*t^4.729 + 2*t^4.906 + 3*t^5.082 + 2*t^5.259 + t^5.436 + 3*t^5.647 + 3*t^5.823 + 2*t^6. + 2*t^6.177 + t^6.353 + t^6.564 + 3*t^6.741 + 5*t^6.918 + 5*t^7.094 + 5*t^7.271 + 3*t^7.447 + 5*t^7.624 + 3*t^7.8 + 3*t^7.835 + 2*t^7.977 + 5*t^8.012 + t^8.153 + 5*t^8.188 - t^8.365 - t^8.541 + t^8.753 + 3*t^8.929 - t^4.271/y - t^6.459/y - (2*t^6.812)/y - t^6.988/y + (2*t^7.553)/y + (4*t^7.729)/y + (3*t^7.906)/y + (3*t^8.082)/y + (2*t^8.259)/y + t^8.647/y + (4*t^8.823)/y - t^4.271*y - t^6.459*y - 2*t^6.812*y - t^6.988*y + 2*t^7.553*y + 4*t^7.729*y + 3*t^7.906*y + 3*t^8.082*y + 2*t^8.259*y + t^8.647*y + 4*t^8.823*y g1^6*t^2.188 + g1*t^2.365 + (2*t^2.541)/g1^4 + t^2.718/g1^9 + 2*g1^4*t^3.459 + (2*t^3.635)/g1 + g1^12*t^4.376 + 3*g1^7*t^4.553 + 4*g1^2*t^4.729 + (2*t^4.906)/g1^3 + (3*t^5.082)/g1^8 + (2*t^5.259)/g1^13 + t^5.436/g1^18 + 3*g1^10*t^5.647 + 3*g1^5*t^5.823 + 2*t^6. + (2*t^6.177)/g1^5 + t^6.353/g1^10 + g1^18*t^6.564 + 3*g1^13*t^6.741 + 5*g1^8*t^6.918 + 5*g1^3*t^7.094 + (5*t^7.271)/g1^2 + (3*t^7.447)/g1^7 + (5*t^7.624)/g1^12 + (3*t^7.8)/g1^17 + 3*g1^16*t^7.835 + (2*t^7.977)/g1^22 + 5*g1^11*t^8.012 + t^8.153/g1^27 + 5*g1^6*t^8.188 - g1*t^8.365 - t^8.541/g1^4 + g1^24*t^8.753 + 3*g1^19*t^8.929 - t^4.271/(g1^2*y) - (g1^4*t^6.459)/y - (2*t^6.812)/(g1^6*y) - t^6.988/(g1^11*y) + (2*g1^7*t^7.553)/y + (4*g1^2*t^7.729)/y + (3*t^7.906)/(g1^3*y) + (3*t^8.082)/(g1^8*y) + (2*t^8.259)/(g1^13*y) + (g1^10*t^8.647)/y + (4*g1^5*t^8.823)/y - (t^4.271*y)/g1^2 - g1^4*t^6.459*y - (2*t^6.812*y)/g1^6 - (t^6.988*y)/g1^11 + 2*g1^7*t^7.553*y + 4*g1^2*t^7.729*y + (3*t^7.906*y)/g1^3 + (3*t^8.082*y)/g1^8 + (2*t^8.259*y)/g1^13 + g1^10*t^8.647*y + 4*g1^5*t^8.823*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
55469 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{2}M_{6}$ 0.6711 0.8492 0.7903 [M:[0.8492, 1.2123, 0.7877, 0.7262, 0.9107, 0.7877], q:[0.7262, 0.4246], qb:[0.3631, 0.7877], phi:[0.4246]] t^2.179 + 2*t^2.363 + 2*t^2.548 + t^2.732 + 2*t^3.452 + t^3.637 + t^4.357 + 4*t^4.542 + 6*t^4.726 + 4*t^4.911 + 4*t^5.095 + 2*t^5.28 + t^5.464 + 3*t^5.631 + 4*t^5.816 + 2*t^6. - t^4.274/y - t^4.274*y detail


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
46638 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ 0.6485 0.8133 0.7973 [M:[0.8791, 1.2198, 0.7802, 0.6813], q:[0.6813, 0.4396], qb:[0.3407, 0.7802], phi:[0.4396]] t^2.044 + t^2.341 + 2*t^2.637 + t^3.066 + 2*t^3.363 + 2*t^3.659 + t^4.088 + 3*t^4.385 + 4*t^4.681 + t^4.978 + t^5.11 + 2*t^5.275 + 4*t^5.407 + 5*t^5.703 + 2*t^6. - t^4.319/y - t^4.319*y detail