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
947 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}^{2}$ + ${ }M_{3}M_{6}$ 0.7067 0.861 0.8208 [M:[1.0, 0.8738, 0.8738, 1.0, 1.0, 1.1262], q:[0.5631, 0.4369], qb:[0.5631, 0.5631], phi:[0.4685]] [M:[[0, 0], [-4, -4], [-6, -2], [2, -2], [-2, 2], [6, 2]], q:[[2, 2], [-2, -2]], qb:[[4, 0], [0, 4]], phi:[[-1, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$ ${}M_{1}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{6}$ -2 t^2.621 + t^2.811 + 3*t^3. + 2*t^3.379 + t^4.027 + 3*t^4.405 + 6*t^4.784 + t^5.243 + t^5.432 + t^5.621 + 3*t^5.811 - 2*t^6. + 2*t^6.189 + 2*t^6.379 + t^6.648 + 3*t^6.757 + t^6.838 + 3*t^7.027 + 2*t^7.216 + 5*t^7.405 + 3*t^7.595 + 12*t^7.784 + t^7.864 - 6*t^7.973 + 2*t^8.054 + 9*t^8.162 + t^8.243 + 4*t^8.432 - 2*t^8.621 + 4*t^8.811 - t^4.405/y - t^7.027/y - t^7.216/y + t^7.595/y + t^7.784/y + t^8.432/y + (3*t^8.621)/y + (3*t^8.811)/y - t^4.405*y - t^7.027*y - t^7.216*y + t^7.595*y + t^7.784*y + t^8.432*y + 3*t^8.621*y + 3*t^8.811*y t^2.621/(g1^4*g2^4) + t^2.811/(g1^2*g2^2) + t^3. + (g1^2*t^3.)/g2^2 + (g2^2*t^3.)/g1^2 + g1^6*g2^2*t^3.379 + g1^2*g2^6*t^3.379 + t^4.027/(g1^5*g2^5) + (g1*t^4.405)/g2^3 + t^4.405/(g1*g2) + (g2*t^4.405)/g1^3 + (g1^7*t^4.784)/g2 + g1^5*g2*t^4.784 + 2*g1^3*g2^3*t^4.784 + g1*g2^5*t^4.784 + (g2^7*t^4.784)/g1 + t^5.243/(g1^8*g2^8) + t^5.432/(g1^6*g2^6) + t^5.621/(g1^4*g2^4) + t^5.811/g1^4 + t^5.811/g2^4 + t^5.811/(g1^2*g2^2) - 2*t^6. + g1^4*t^6.189 + g2^4*t^6.189 + g1^8*t^6.379 + g2^8*t^6.379 + t^6.648/(g1^9*g2^9) + g1^12*g2^4*t^6.757 + g1^8*g2^8*t^6.757 + g1^4*g2^12*t^6.757 + t^6.838/(g1^7*g2^7) + t^7.027/(g1^3*g2^7) + t^7.027/(g1^5*g2^5) + t^7.027/(g1^7*g2^3) + t^7.216/(g1*g2^5) + t^7.216/(g1^5*g2) + (g1^3*t^7.405)/g2^5 + (g1*t^7.405)/g2^3 + t^7.405/(g1*g2) + (g2*t^7.405)/g1^3 + (g2^3*t^7.405)/g1^5 + (g1^5*t^7.595)/g2^3 + g1*g2*t^7.595 + (g2^5*t^7.595)/g1^3 + (g1^9*t^7.784)/g2^3 + (2*g1^7*t^7.784)/g2 + 2*g1^5*g2*t^7.784 + 2*g1^3*g2^3*t^7.784 + 2*g1*g2^5*t^7.784 + (2*g2^7*t^7.784)/g1 + (g2^9*t^7.784)/g1^3 + t^7.864/(g1^12*g2^12) - g1^9*g2*t^7.973 - g1^7*g2^3*t^7.973 - 2*g1^5*g2^5*t^7.973 - g1^3*g2^7*t^7.973 - g1*g2^9*t^7.973 + (2*t^8.054)/(g1^10*g2^10) + g1^13*g2*t^8.162 + g1^11*g2^3*t^8.162 + 2*g1^9*g2^5*t^8.162 + g1^7*g2^7*t^8.162 + 2*g1^5*g2^9*t^8.162 + g1^3*g2^11*t^8.162 + g1*g2^13*t^8.162 + t^8.243/(g1^8*g2^8) + t^8.432/(g1^4*g2^8) + (2*t^8.432)/(g1^6*g2^6) + t^8.432/(g1^8*g2^4) - (2*t^8.621)/(g1^4*g2^4) + t^8.811/g1^4 + (g1^2*t^8.811)/g2^6 + t^8.811/g2^4 + (g2^2*t^8.811)/g1^6 - t^4.405/(g1*g2*y) - t^7.027/(g1^5*g2^5*y) - t^7.216/(g1^3*g2^3*y) + (g1*g2*t^7.595)/y + (g1^3*g2^3*t^7.784)/y + t^8.432/(g1^6*g2^6*y) + t^8.621/(g1^2*g2^6*y) + t^8.621/(g1^4*g2^4*y) + t^8.621/(g1^6*g2^2*y) + t^8.811/(g1^4*y) + t^8.811/(g2^4*y) + t^8.811/(g1^2*g2^2*y) - (t^4.405*y)/(g1*g2) - (t^7.027*y)/(g1^5*g2^5) - (t^7.216*y)/(g1^3*g2^3) + g1*g2*t^7.595*y + g1^3*g2^3*t^7.784*y + (t^8.432*y)/(g1^6*g2^6) + (t^8.621*y)/(g1^2*g2^6) + (t^8.621*y)/(g1^4*g2^4) + (t^8.621*y)/(g1^6*g2^2) + (t^8.811*y)/g1^4 + (t^8.811*y)/g2^4 + (t^8.811*y)/(g1^2*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


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
598 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}^{2}$ 0.7203 0.8855 0.8134 [M:[1.0, 0.8402, 0.8171, 1.0231, 0.9769], q:[0.5799, 0.4201], qb:[0.603, 0.5568], phi:[0.4601]] t^2.451 + t^2.521 + t^2.76 + t^2.931 + t^3. + t^3.069 + t^3.41 + t^3.901 + t^4.311 + t^4.38 + t^4.449 + t^4.721 + t^4.79 + 2*t^4.859 + t^4.903 + t^4.929 + t^4.972 + t^4.998 + t^5.041 + t^5.212 + t^5.281 + t^5.382 + t^5.451 + 2*t^5.521 + t^5.691 + t^5.76 + t^5.83 + t^5.861 - 2*t^6. - t^4.38/y - t^4.38*y detail