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
61256 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ 1.3213 1.5664 0.8436 [X:[], M:[0.8, 1.2791], q:[0.586, 0.4279], qb:[0.293, 0.293], phi:[0.4]] [X:[], M:[[0], [3]], q:[[2], [-4]], qb:[[1], [1]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{3}$ 3 t^2.16 + 2*t^2.4 + 2*t^2.64 + 2*t^3.36 + 5*t^3.84 + t^4.33 + 4*t^4.56 + 5*t^4.8 + 8*t^5.04 + 3*t^5.27 + 2*t^5.53 + 4*t^5.76 + 3*t^6. + 14*t^6.24 + 8*t^6.47 + t^6.49 + 7*t^6.73 + 7*t^6.96 + 16*t^7.2 + 13*t^7.44 + t^7.45 + 23*t^7.67 + 2*t^7.69 + 4*t^7.91 + 8*t^7.93 + 5*t^8.16 + 16*t^8.4 + 17*t^8.64 + t^8.65 + 36*t^8.87 + 5*t^8.89 - t^4.2/y - t^5.4/y - t^6.36/y - (2*t^6.6)/y - (2*t^6.84)/y + t^7.56/y + (2*t^7.8)/y + t^8.04/y + t^8.27/y + t^8.53/y - t^4.2*y - t^5.4*y - t^6.36*y - 2*t^6.6*y - 2*t^6.84*y + t^7.56*y + 2*t^7.8*y + t^8.04*y + t^8.27*y + t^8.53*y t^2.16/g1^3 + 2*t^2.4 + 2*g1^3*t^2.64 + (2*t^3.36)/g1^3 + 5*g1^3*t^3.84 + t^4.33/g1^6 + (4*t^4.56)/g1^3 + 5*t^4.8 + 8*g1^3*t^5.04 + 3*g1^6*t^5.27 + (2*t^5.53)/g1^6 + (4*t^5.76)/g1^3 + 3*t^6. + 14*g1^3*t^6.24 + 8*g1^6*t^6.47 + t^6.49/g1^9 + (7*t^6.73)/g1^6 + (7*t^6.96)/g1^3 + 16*t^7.2 + 13*g1^3*t^7.44 + t^7.45/g1^12 + 23*g1^6*t^7.67 + (2*t^7.69)/g1^9 + 4*g1^9*t^7.91 + (8*t^7.93)/g1^6 + (5*t^8.16)/g1^3 + 16*t^8.4 + 17*g1^3*t^8.64 + t^8.65/g1^12 + 36*g1^6*t^8.87 + (5*t^8.89)/g1^9 - t^4.2/y - t^5.4/y - t^6.36/(g1^3*y) - (2*t^6.6)/y - (2*g1^3*t^6.84)/y + t^7.56/(g1^3*y) + (2*t^7.8)/y + (g1^3*t^8.04)/y + (g1^6*t^8.27)/y + t^8.53/(g1^6*y) - t^4.2*y - t^5.4*y - (t^6.36*y)/g1^3 - 2*t^6.6*y - 2*g1^3*t^6.84*y + (t^7.56*y)/g1^3 + 2*t^7.8*y + g1^3*t^8.04*y + g1^6*t^8.27*y + (t^8.53*y)/g1^6


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
58793 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ 1.3214 1.5667 0.8434 [X:[], M:[0.8, 1.2745], q:[0.5858, 0.4283], qb:[0.2971, 0.2887], phi:[0.4]] t^2.15 + 2*t^2.4 + t^2.62 + t^2.65 + t^3.35 + t^3.38 + 3*t^3.82 + 2*t^3.85 + t^4.3 + 3*t^4.55 + t^4.58 + t^4.77 + 4*t^4.8 + 4*t^5.02 + 4*t^5.05 + t^5.25 + t^5.27 + t^5.3 + t^5.5 + t^5.53 + 2*t^5.75 + 2*t^5.78 + 3*t^5.97 - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail