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
46648 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ 0.5879 0.7303 0.805 [M:[0.6886, 1.0329, 0.9671, 0.7545], q:[1.1392, 0.5165], qb:[0.4506, 0.5165], phi:[0.3443]] [M:[[4], [6], [-6], [16]], q:[[-5], [3]], qb:[[-9], [3]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ ${}$ -2 2*t^2.066 + t^2.263 + 2*t^2.901 + t^3.099 + 4*t^4.132 + 2*t^4.329 + t^4.527 + t^4.77 + 5*t^4.967 + 3*t^5.165 + t^5.362 + 2*t^5.802 - 2*t^6. + 5*t^6.198 + 4*t^6.395 + 2*t^6.593 + t^6.79 - t^6.835 + 7*t^7.033 + 6*t^7.23 + 3*t^7.428 + t^7.626 + t^7.671 + 2*t^7.868 - 4*t^8.066 + 5*t^8.263 + 5*t^8.461 + 4*t^8.658 + 2*t^8.856 - 8*t^8.901 - t^4.033/y - (2*t^6.099)/y - t^6.296/y + t^7.132/y + (2*t^7.329)/y + t^7.77/y + (6*t^7.967)/y + t^8.165/y - t^8.362/y - t^8.56/y + t^8.802/y - t^4.033*y - 2*t^6.099*y - t^6.296*y + t^7.132*y + 2*t^7.329*y + t^7.77*y + 6*t^7.967*y + t^8.165*y - t^8.362*y - t^8.56*y + t^8.802*y 2*g1^4*t^2.066 + g1^16*t^2.263 + (2*t^2.901)/g1^6 + g1^6*t^3.099 + 4*g1^8*t^4.132 + 2*g1^20*t^4.329 + g1^32*t^4.527 + t^4.77/g1^14 + (5*t^4.967)/g1^2 + 3*g1^10*t^5.165 + g1^22*t^5.362 + (2*t^5.802)/g1^12 - 2*t^6. + 5*g1^12*t^6.198 + 4*g1^24*t^6.395 + 2*g1^36*t^6.593 + g1^48*t^6.79 - t^6.835/g1^10 + 7*g1^2*t^7.033 + 6*g1^14*t^7.23 + 3*g1^26*t^7.428 + g1^38*t^7.626 + t^7.671/g1^20 + (2*t^7.868)/g1^8 - 4*g1^4*t^8.066 + 5*g1^16*t^8.263 + 5*g1^28*t^8.461 + 4*g1^40*t^8.658 + 2*g1^52*t^8.856 - (8*t^8.901)/g1^6 - (g1^2*t^4.033)/y - (2*g1^6*t^6.099)/y - (g1^18*t^6.296)/y + (g1^8*t^7.132)/y + (2*g1^20*t^7.329)/y + t^7.77/(g1^14*y) + (6*t^7.967)/(g1^2*y) + (g1^10*t^8.165)/y - (g1^22*t^8.362)/y - (g1^34*t^8.56)/y + t^8.802/(g1^12*y) - g1^2*t^4.033*y - 2*g1^6*t^6.099*y - g1^18*t^6.296*y + g1^8*t^7.132*y + 2*g1^20*t^7.329*y + (t^7.77*y)/g1^14 + (6*t^7.967*y)/g1^2 + g1^10*t^8.165*y - g1^22*t^8.362*y - g1^34*t^8.56*y + (t^8.802*y)/g1^12


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
47142 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{5}$ 0.5915 0.7355 0.8042 [M:[0.6962, 1.0443, 0.9557, 0.7848, 0.9557], q:[1.1298, 0.5221], qb:[0.4336, 0.5221], phi:[0.3481]] 2*t^2.089 + t^2.354 + 3*t^2.867 + 4*t^4.177 + 2*t^4.443 + t^4.69 + t^4.709 + 7*t^4.956 + 2*t^5.221 + 5*t^5.734 - 4*t^6. - t^4.044/y - t^4.044*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
46218 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ 0.5703 0.6987 0.8162 [M:[0.7028, 1.0541, 0.9459], q:[1.1215, 0.5271], qb:[0.4188, 0.5271], phi:[0.3514]] 2*t^2.108 + 2*t^2.838 + t^3.162 + t^3.567 + 4*t^4.217 + t^4.621 + 5*t^4.946 + t^5.271 + 4*t^5.675 - 2*t^6. - t^4.054/y - t^4.054*y detail