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
202 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ 0.7121 0.8517 0.8362 [M:[0.8744, 1.1256, 1.1256, 0.8278], q:[0.5861, 0.5395], qb:[0.5861, 0.5395], phi:[0.4372]] [M:[[0, -2, -2], [0, 2, 2], [0, 2, 2], [1, -4, -2]], q:[[-1, 2, 2], [1, 0, 0]], qb:[[0, 2, 0], [0, 0, 2]], phi:[[0, -1, -1]]] 3
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ ${}$ -8 t^2.483 + t^3.237 + 5*t^3.377 + 3*t^4.549 + 4*t^4.688 + 3*t^4.828 + t^4.967 + t^5.72 + t^5.86 - 8*t^6. - 4*t^6.14 + t^6.474 + 5*t^6.614 + 14*t^6.754 + 3*t^7.032 - 4*t^7.312 + t^7.45 - 4*t^7.451 + 3*t^7.786 + 12*t^7.925 + 12*t^8.065 + t^8.204 + 8*t^8.205 + t^8.344 - 5*t^8.483 + 3*t^8.763 + t^8.958 - t^4.312/y - t^6.795/y + t^7.828/y + t^8.72/y + (5*t^8.86)/y - t^4.312*y - t^6.795*y + t^7.828*y + t^8.72*y + 5*t^8.86*y (g1*t^2.483)/(g2^4*g3^2) + g1*g3^2*t^3.237 + g1*g2^2*t^3.377 + 3*g2^2*g3^2*t^3.377 + (g2^2*g3^4*t^3.377)/g1 + (g1^2*t^4.549)/(g2*g3) + (g1*g3*t^4.549)/g2 + (g3^3*t^4.549)/g2 + (g1*g2*t^4.688)/g3 + 2*g2*g3*t^4.688 + (g2*g3^3*t^4.688)/g1 + (g2^3*t^4.828)/g3 + (g2^3*g3*t^4.828)/g1 + (g2^3*g3^3*t^4.828)/g1^2 + (g1^2*t^4.967)/(g2^8*g3^4) + (g1^2*t^5.72)/g2^4 + (g1*t^5.86)/g2^2 - 4*t^6. - (2*g1*t^6.)/g3^2 - (2*g3^2*t^6.)/g1 - (2*g2^2*t^6.14)/g1 - (g2^2*t^6.14)/g3^2 - (g2^2*g3^2*t^6.14)/g1^2 + g1^2*g3^4*t^6.474 + g1^2*g2^2*g3^2*t^6.614 + 3*g1*g2^2*g3^4*t^6.614 + g2^2*g3^6*t^6.614 + g1^2*g2^4*t^6.754 + 3*g1*g2^4*g3^2*t^6.754 + 6*g2^4*g3^4*t^6.754 + (3*g2^4*g3^6*t^6.754)/g1 + (g2^4*g3^8*t^6.754)/g1^2 + (g1^3*t^7.032)/(g2^5*g3^3) + (g1^2*t^7.032)/(g2^5*g3) + (g1*g3*t^7.032)/g2^5 - (g1*t^7.312)/(g2*g3^3) - (2*t^7.312)/(g2*g3) - (g3*t^7.312)/(g1*g2) + (g1^3*t^7.45)/(g2^12*g3^6) - (g2*t^7.451)/g3^3 - (2*g2*t^7.451)/(g1*g3) - (g2*g3*t^7.451)/g1^2 + (g1^3*g3*t^7.786)/g2 + (g1^2*g3^3*t^7.786)/g2 + (g1*g3^5*t^7.786)/g2 + (g1^3*g2*t^7.925)/g3 + 3*g1^2*g2*g3*t^7.925 + 4*g1*g2*g3^3*t^7.925 + 3*g2*g3^5*t^7.925 + (g2*g3^7*t^7.925)/g1 + (g1^2*g2^3*t^8.065)/g3 + 3*g1*g2^3*g3*t^8.065 + 4*g2^3*g3^3*t^8.065 + (3*g2^3*g3^5*t^8.065)/g1 + (g2^3*g3^7*t^8.065)/g1^2 + (g1^3*t^8.204)/(g2^8*g3^2) + (g1*g2^5*t^8.205)/g3 + 2*g2^5*g3*t^8.205 + (2*g2^5*g3^3*t^8.205)/g1 + (2*g2^5*g3^5*t^8.205)/g1^2 + (g2^5*g3^7*t^8.205)/g1^3 + (g1^2*t^8.344)/(g2^6*g3^2) - t^8.483/g2^4 - (g1^2*t^8.483)/(g2^4*g3^4) - (3*g1*t^8.483)/(g2^4*g3^2) + t^8.763/g1^2 + t^8.763/g3^4 + t^8.763/(g1*g3^2) + (g1^3*g3^2*t^8.958)/g2^4 - t^4.312/(g2*g3*y) - (g1*t^6.795)/(g2^5*g3^3*y) + (g2^3*g3*t^7.828)/(g1*y) + (g1^2*t^8.72)/(g2^4*y) + (3*g1*t^8.86)/(g2^2*y) + (g1^2*t^8.86)/(g2^2*g3^2*y) + (g3^2*t^8.86)/(g2^2*y) - (t^4.312*y)/(g2*g3) - (g1*t^6.795*y)/(g2^5*g3^3) + (g2^3*g3*t^7.828*y)/g1 + (g1^2*t^8.72*y)/g2^4 + (3*g1*t^8.86*y)/g2^2 + (g1^2*t^8.86*y)/(g2^2*g3^2) + (g3^2*t^8.86*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


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
55769 SU2adj1nf3 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}$ + ${ }M_{2}q_{3}\tilde{q}_{1}$ 0.7121 0.8517 0.8362 [M:[1.1256, 0.8278], q:[0.7814, 1.2186, 0.5861], qb:[0.5861, 0.5395, 0.5395], phi:[0.4372]] t^2.483 + t^3.237 + 5*t^3.377 + 3*t^4.549 + 4*t^4.688 + 3*t^4.828 + t^4.967 + t^5.72 + t^5.86 - 8*t^6. - t^4.312/y - t^4.312*y detail


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
123 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ 0.7003 0.8367 0.837 [M:[0.9093, 1.0907, 1.0907], q:[0.5454, 0.5454], qb:[0.5454, 0.5454], phi:[0.4546]] 7*t^3.272 + 10*t^4.636 - 16*t^6. - t^4.364/y - t^4.364*y detail