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
46262 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ 0.608 0.7809 0.7786 [M:[0.9776, 0.7444, 1.0673], q:[0.7444, 0.2781], qb:[0.4663, 0.4663], phi:[0.5112]] [M:[[4], [1], [-12]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ ${}$ -2 3*t^2.233 + t^2.933 + t^3.067 + 2*t^3.202 + 2*t^3.632 + t^3.767 + 3*t^4.332 + 6*t^4.466 + 3*t^5.166 + 3*t^5.3 + 4*t^5.435 + 6*t^5.865 - 2*t^6. + t^6.135 + 2*t^6.269 + 3*t^6.404 + 7*t^6.565 + 9*t^6.7 + t^6.834 + 3*t^7.264 + 6*t^7.399 + 5*t^7.534 + 6*t^7.668 + 4*t^7.964 + 9*t^8.099 - 9*t^8.233 + t^8.368 + 4*t^8.502 + 5*t^8.637 + 5*t^8.663 + 12*t^8.798 + 7*t^8.933 - t^4.534/y - t^6.767/y + t^7.332/y + (3*t^7.466)/y - t^7.736/y + (3*t^8.166)/y + (4*t^8.3)/y + (6*t^8.435)/y + (6*t^8.865)/y - t^4.534*y - t^6.767*y + t^7.332*y + 3*t^7.466*y - t^7.736*y + 3*t^8.166*y + 4*t^8.3*y + 6*t^8.435*y + 6*t^8.865*y 3*g1*t^2.233 + g1^4*t^2.933 + t^3.067/g1^4 + (2*t^3.202)/g1^12 + 2*g1^7*t^3.632 + t^3.767/g1 + 3*g1^10*t^4.332 + 6*g1^2*t^4.466 + 3*g1^5*t^5.166 + (3*t^5.3)/g1^3 + (4*t^5.435)/g1^11 + 6*g1^8*t^5.865 - 2*t^6. + t^6.135/g1^8 + (2*t^6.269)/g1^16 + (3*t^6.404)/g1^24 + 7*g1^11*t^6.565 + 9*g1^3*t^6.7 + t^6.834/g1^5 + 3*g1^14*t^7.264 + 6*g1^6*t^7.399 + (5*t^7.534)/g1^2 + (6*t^7.668)/g1^10 + 4*g1^17*t^7.964 + 9*g1^9*t^8.099 - 9*g1*t^8.233 + t^8.368/g1^7 + (4*t^8.502)/g1^15 + (5*t^8.637)/g1^23 + 5*g1^20*t^8.663 + 12*g1^12*t^8.798 + 7*g1^4*t^8.933 - t^4.534/(g1^2*y) - t^6.767/(g1*y) + (g1^10*t^7.332)/y + (3*g1^2*t^7.466)/y - t^7.736/(g1^14*y) + (3*g1^5*t^8.166)/y + (4*t^8.3)/(g1^3*y) + (6*t^8.435)/(g1^11*y) + (6*g1^8*t^8.865)/y - (t^4.534*y)/g1^2 - (t^6.767*y)/g1 + g1^10*t^7.332*y + 3*g1^2*t^7.466*y - (t^7.736*y)/g1^14 + 3*g1^5*t^8.166*y + (4*t^8.3*y)/g1^3 + (6*t^8.435*y)/g1^11 + 6*g1^8*t^8.865*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
45966 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ 0.6081 0.7817 0.778 [M:[0.9777, 0.7349, 1.0669], q:[0.7444, 0.2779], qb:[0.4761, 0.457], phi:[0.5112]] 2*t^2.205 + t^2.262 + t^2.933 + t^3.067 + 2*t^3.201 + t^3.604 + t^3.662 + t^3.738 + t^4.275 + t^4.333 + t^4.39 + 3*t^4.409 + 2*t^4.467 + t^4.524 + 2*t^5.138 + t^5.195 + 2*t^5.272 + t^5.329 + 3*t^5.405 + t^5.463 + 2*t^5.809 + 3*t^5.866 + t^5.923 + t^5.943 - 2*t^6. - t^4.533/y - t^4.533*y detail