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
46755 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{2}M_{3}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ 0.5221 0.6729 0.7759 [M:[0.8043, 0.7935, 1.2065, 0.7935], q:[0.5924, 1.0054], qb:[0.2011, 0.5924], phi:[0.4022]] [M:[[-4], [6], [-6], [6]], q:[[7], [-5]], qb:[[-1], [7]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{4}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$ ${}$ -5 3*t^2.38 + 3*t^2.413 + t^3.554 + 7*t^4.761 + 10*t^4.793 + 5*t^4.826 + 3*t^5.935 + t^5.967 - 5*t^6. - 2*t^6.033 + t^7.109 + 12*t^7.141 + 18*t^7.174 + 13*t^7.207 + 6*t^7.239 + 7*t^8.315 + 2*t^8.348 - 18*t^8.38 - 18*t^8.413 - 5*t^8.446 - t^4.207/y - t^6.587/y - (2*t^6.62)/y + (3*t^7.761)/y + (11*t^7.793)/y + (4*t^7.826)/y + (3*t^8.935)/y + (2*t^8.967)/y - t^4.207*y - t^6.587*y - 2*t^6.62*y + 3*t^7.761*y + 11*t^7.793*y + 4*t^7.826*y + 3*t^8.935*y + 2*t^8.967*y 3*g1^6*t^2.38 + (3*t^2.413)/g1^4 + g1^14*t^3.554 + 7*g1^12*t^4.761 + 10*g1^2*t^4.793 + (5*t^4.826)/g1^8 + 3*g1^20*t^5.935 + g1^10*t^5.967 - 5*t^6. - (2*t^6.033)/g1^10 + g1^28*t^7.109 + 12*g1^18*t^7.141 + 18*g1^8*t^7.174 + (13*t^7.207)/g1^2 + (6*t^7.239)/g1^12 + 7*g1^26*t^8.315 + 2*g1^16*t^8.348 - 18*g1^6*t^8.38 - (18*t^8.413)/g1^4 - (5*t^8.446)/g1^14 - t^4.207/(g1^2*y) - (g1^4*t^6.587)/y - (2*t^6.62)/(g1^6*y) + (3*g1^12*t^7.761)/y + (11*g1^2*t^7.793)/y + (4*t^7.826)/(g1^8*y) + (3*g1^20*t^8.935)/y + (2*g1^10*t^8.967)/y - (t^4.207*y)/g1^2 - g1^4*t^6.587*y - (2*t^6.62*y)/g1^6 + 3*g1^12*t^7.761*y + 11*g1^2*t^7.793*y + (4*t^7.826*y)/g1^8 + 3*g1^20*t^8.935*y + 2*g1^10*t^8.967*y


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
46092 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{2}M_{3}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ 0.5056 0.6427 0.7867 [M:[0.7952, 0.8071, 1.1929], q:[0.6083, 0.9941], qb:[0.1988, 0.6083], phi:[0.3976]] 3*t^2.386 + 2*t^2.421 + t^3.579 + t^3.65 + 5*t^4.771 + 7*t^4.807 + 4*t^4.843 + t^5.964 - 3*t^6. - t^4.193/y - t^4.193*y detail