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
517 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{4}M_{5}$ 0.7103 0.8687 0.8177 [M:[0.9326, 0.9326, 0.9326, 1.0674, 0.9326], q:[0.6011, 0.4663], qb:[0.4663, 0.6011], phi:[0.4663]] [M:[[-2, -2], [-8, -4], [4, 0], [2, 2], [-2, -2]], q:[[6, 4], [-4, -2]], qb:[[2, 0], [0, 2]], phi:[[-1, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{3}\phi_{1}^{2}$ ${}M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ -3 5*t^2.798 + t^3.202 + t^3.606 + 3*t^4.197 + 4*t^4.601 + 3*t^5.005 + 11*t^5.596 - 3*t^6. + t^6.404 + t^6.808 + 11*t^6.995 + t^7.213 + 9*t^7.399 + 7*t^7.803 + 23*t^8.394 + 3*t^8.612 - 14*t^8.798 - t^4.399/y - (4*t^7.197)/y + (4*t^7.601)/y + (10*t^8.596)/y - t^4.399*y - 4*t^7.197*y + 4*t^7.601*y + 10*t^8.596*y g1^4*t^2.798 + t^2.798/(g1^8*g2^4) + (3*t^2.798)/(g1^2*g2^2) + g1^2*g2^2*t^3.202 + g1^6*g2^6*t^3.606 + t^4.197/(g1^9*g2^5) + t^4.197/(g1^3*g2^3) + (g1^3*t^4.197)/g2 + t^4.601/(g1^5*g2) + 2*g1*g2*t^4.601 + g1^7*g2^3*t^4.601 + (g2^3*t^5.005)/g1 + g1^5*g2^5*t^5.005 + g1^11*g2^7*t^5.005 + g1^8*t^5.596 + t^5.596/(g1^16*g2^8) + (2*t^5.596)/(g1^10*g2^6) + (5*t^5.596)/(g1^4*g2^4) + (2*g1^2*t^5.596)/g2^2 - t^6. - t^6./(g1^6*g2^2) - g1^6*g2^2*t^6. + g1^4*g2^4*t^6.404 + g1^8*g2^8*t^6.808 + t^6.995/(g1^17*g2^9) + (3*t^6.995)/(g1^11*g2^7) + (3*t^6.995)/(g1^5*g2^5) + (3*g1*t^6.995)/g2^3 + (g1^7*t^6.995)/g2 + g1^12*g2^12*t^7.213 + t^7.399/(g1^13*g2^5) + (2*t^7.399)/(g1^7*g2^3) + (3*t^7.399)/(g1*g2) + 2*g1^5*g2*t^7.399 + g1^11*g2^3*t^7.399 + t^7.803/(g1^9*g2) + (2*g2*t^7.803)/g1^3 + g1^3*g2^3*t^7.803 + 2*g1^9*g2^5*t^7.803 + g1^15*g2^7*t^7.803 + g1^12*t^8.394 + t^8.394/(g1^24*g2^12) + (3*t^8.394)/(g1^18*g2^10) + (4*t^8.394)/(g1^12*g2^8) + (7*t^8.394)/(g1^6*g2^6) + (4*t^8.394)/g2^4 + (3*g1^6*t^8.394)/g2^2 + g1^5*g2^9*t^8.612 + g1^11*g2^11*t^8.612 + g1^17*g2^13*t^8.612 - 4*g1^4*t^8.798 - (4*t^8.798)/(g1^8*g2^4) - (6*t^8.798)/(g1^2*g2^2) - t^4.399/(g1*g2*y) - t^7.197/(g1^9*g2^5*y) - (2*t^7.197)/(g1^3*g2^3*y) - (g1^3*t^7.197)/(g2*y) + t^7.601/(g1^5*g2*y) + (2*g1*g2*t^7.601)/y + (g1^7*g2^3*t^7.601)/y + (3*t^8.596)/(g1^10*g2^6*y) + (4*t^8.596)/(g1^4*g2^4*y) + (3*g1^2*t^8.596)/(g2^2*y) - (t^4.399*y)/(g1*g2) - (t^7.197*y)/(g1^9*g2^5) - (2*t^7.197*y)/(g1^3*g2^3) - (g1^3*t^7.197*y)/g2 + (t^7.601*y)/(g1^5*g2) + 2*g1*g2*t^7.601*y + g1^7*g2^3*t^7.601*y + (3*t^8.596*y)/(g1^10*g2^6) + (4*t^8.596*y)/(g1^4*g2^4) + (3*g1^2*t^8.596*y)/g2^2


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
807 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{4}M_{5}$ + ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ 0.7171 0.8807 0.8142 [M:[0.9214, 0.9214, 0.9214, 1.0786, 0.9214, 0.9214], q:[0.6179, 0.4607], qb:[0.4607, 0.6179], phi:[0.4607]] 6*t^2.764 + t^3.707 + 3*t^4.146 + 4*t^4.618 + 3*t^5.09 + 17*t^5.528 - 8*t^6. - t^4.382/y - t^4.382*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
330 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ 0.7046 0.8591 0.8202 [M:[0.9439, 0.9439, 0.9439, 1.0561], q:[0.5841, 0.472], qb:[0.472, 0.5841], phi:[0.472]] 4*t^2.832 + 2*t^3.168 + t^3.505 + 3*t^4.248 + 4*t^4.584 + 3*t^4.921 + 6*t^5.664 - t^4.416/y - t^4.416*y detail