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
1663 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{6}$ + ${ }M_{2}M_{7}$ 0.648 0.8137 0.7964 [M:[0.8252, 1.2, 0.7748, 0.8, 0.7748, 1.1748, 0.8], q:[0.8, 0.3748], qb:[0.8, 0.4252], phi:[0.4]] [M:[[1], [0], [-1], [0], [-1], [-1], [0]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{5}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{6}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{3}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{7}q_{1}q_{2}$ ${}\phi_{1}\tilde{q}_{1}^{2}$ -3 2*t^2.324 + 3*t^2.4 + t^3.449 + 2*t^3.524 + t^3.751 + 3*t^4.649 + 6*t^4.724 + 7*t^4.8 + 2*t^5.773 + 6*t^5.849 + 4*t^5.924 - 3*t^6. + 2*t^6.151 + t^6.898 + 6*t^6.973 + 10*t^7.049 + 10*t^7.124 + 9*t^7.2 - 2*t^7.276 - 2*t^7.351 + t^7.502 + 3*t^8.098 + 10*t^8.173 + 11*t^8.249 - 11*t^8.4 - 4*t^8.476 + 3*t^8.551 - t^4.2/y - (2*t^6.524)/y - (2*t^6.6)/y + t^7.649/y + (6*t^7.724)/y + (5*t^7.8)/y + (2*t^7.876)/y + (2*t^8.773)/y + (4*t^8.849)/y + (2*t^8.924)/y - t^4.2*y - 2*t^6.524*y - 2*t^6.6*y + t^7.649*y + 6*t^7.724*y + 5*t^7.8*y + 2*t^7.876*y + 2*t^8.773*y + 4*t^8.849*y + 2*t^8.924*y (2*t^2.324)/g1 + 3*t^2.4 + t^3.449/g1^2 + (2*t^3.524)/g1 + g1^2*t^3.751 + (3*t^4.649)/g1^2 + (6*t^4.724)/g1 + 7*t^4.8 + (2*t^5.773)/g1^3 + (6*t^5.849)/g1^2 + (4*t^5.924)/g1 - 3*t^6. + 2*g1^2*t^6.151 + t^6.898/g1^4 + (6*t^6.973)/g1^3 + (10*t^7.049)/g1^2 + (10*t^7.124)/g1 + 9*t^7.2 - 2*g1*t^7.276 - 2*g1^2*t^7.351 + g1^4*t^7.502 + (3*t^8.098)/g1^4 + (10*t^8.173)/g1^3 + (11*t^8.249)/g1^2 - 11*t^8.4 - 4*g1*t^8.476 + 3*g1^2*t^8.551 - t^4.2/y - (2*t^6.524)/(g1*y) - (2*t^6.6)/y + t^7.649/(g1^2*y) + (6*t^7.724)/(g1*y) + (5*t^7.8)/y + (2*g1*t^7.876)/y + (2*t^8.773)/(g1^3*y) + (4*t^8.849)/(g1^2*y) + (2*t^8.924)/(g1*y) - t^4.2*y - (2*t^6.524*y)/g1 - 2*t^6.6*y + (t^7.649*y)/g1^2 + (6*t^7.724*y)/g1 + 5*t^7.8*y + 2*g1*t^7.876*y + (2*t^8.773*y)/g1^3 + (4*t^8.849*y)/g1^2 + (2*t^8.924*y)/g1


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
1069 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{6}$ 0.6315 0.7847 0.8048 [M:[0.8252, 1.2, 0.7748, 0.8, 0.7748, 1.1748], q:[0.8, 0.3748], qb:[0.8, 0.4252], phi:[0.4]] 2*t^2.324 + 2*t^2.4 + t^3.449 + 2*t^3.524 + t^3.6 + t^3.751 + 3*t^4.649 + 4*t^4.724 + 4*t^4.8 + 2*t^5.773 + 5*t^5.849 + 4*t^5.924 - t^6. - t^4.2/y - t^4.2*y detail