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
58450 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$ 1.427 1.6905 0.8441 [X:[], M:[0.7839], q:[0.4107, 0.3946], qb:[0.4054, 0.3893], phi:[0.4]] [X:[], M:[[3]], q:[[-2], [1]], qb:[[-1], [2]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${2}\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ 2}\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ 3}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ 8 2*t^2.35 + 3*t^2.4 + t^2.45 + t^3.55 + 3*t^3.6 + 3*t^4.7 + 8*t^4.75 + 12*t^4.8 + 5*t^4.85 + t^4.9 + 2*t^5.9 + 8*t^5.95 + 8*t^6. + 2*t^6.05 + 4*t^7.06 + 15*t^7.1 + 30*t^7.15 + 34*t^7.2 + 16*t^7.25 + 6*t^7.3 + t^7.34 + 3*t^8.26 + 14*t^8.3 + 20*t^8.35 + 17*t^8.4 + 2*t^8.45 + t^8.5 - t^4.2/y - t^5.4/y - (2*t^6.55)/y - (3*t^6.6)/y - t^6.65/y + t^7.7/y + (4*t^7.75)/y + (2*t^7.8)/y + (3*t^7.85)/y - t^8.9/y + (2*t^8.95)/y - t^4.2*y - t^5.4*y - 2*t^6.55*y - 3*t^6.6*y - t^6.65*y + t^7.7*y + 4*t^7.75*y + 2*t^7.8*y + 3*t^7.85*y - t^8.9*y + 2*t^8.95*y 2*g1^3*t^2.35 + 3*t^2.4 + t^2.45/g1^3 + g1^3*t^3.55 + 3*t^3.6 + 3*g1^6*t^4.7 + 8*g1^3*t^4.75 + 12*t^4.8 + (5*t^4.85)/g1^3 + t^4.9/g1^6 + 2*g1^6*t^5.9 + 8*g1^3*t^5.95 + 8*t^6. + (2*t^6.05)/g1^3 + 4*g1^9*t^7.06 + 15*g1^6*t^7.1 + 30*g1^3*t^7.15 + 34*t^7.2 + (16*t^7.25)/g1^3 + (6*t^7.3)/g1^6 + t^7.34/g1^9 + 3*g1^9*t^8.26 + 14*g1^6*t^8.3 + 20*g1^3*t^8.35 + 17*t^8.4 + (2*t^8.45)/g1^3 + t^8.5/g1^6 - t^4.2/y - t^5.4/y - (2*g1^3*t^6.55)/y - (3*t^6.6)/y - t^6.65/(g1^3*y) + (g1^6*t^7.7)/y + (4*g1^3*t^7.75)/y + (2*t^7.8)/y + (3*t^7.85)/(g1^3*y) - (g1^6*t^8.9)/y + (2*g1^3*t^8.95)/y - t^4.2*y - t^5.4*y - 2*g1^3*t^6.55*y - 3*t^6.6*y - (t^6.65*y)/g1^3 + g1^6*t^7.7*y + 4*g1^3*t^7.75*y + 2*t^7.8*y + (3*t^7.85*y)/g1^3 - g1^6*t^8.9*y + 2*g1^3*t^8.95*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
60990 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ 1.4105 1.6615 0.8489 [X:[], M:[0.7839, 1.2], q:[0.4107, 0.3946], qb:[0.4054, 0.3893], phi:[0.4]] 2*t^2.35 + 2*t^2.4 + t^2.45 + t^3.55 + 4*t^3.6 + 3*t^4.7 + 6*t^4.75 + 9*t^4.8 + 4*t^4.85 + t^4.9 + 2*t^5.9 + 9*t^5.95 + 7*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail


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
57351 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ 1.427 1.6905 0.8441 [M:[0.7838], q:[0.4098, 0.3951], qb:[0.4065, 0.3887], phi:[0.4]] 2*t^2.351 + t^2.395 + t^2.4 + t^2.405 + t^2.449 + t^3.551 + t^3.595 + t^3.6 + t^3.605 + 3*t^4.703 + 2*t^4.747 + 4*t^4.751 + 2*t^4.756 + t^4.791 + 2*t^4.795 + 5*t^4.8 + 3*t^4.805 + t^4.809 + 2*t^4.844 + 2*t^4.849 + t^4.853 + t^4.897 + 2*t^5.903 + 2*t^5.947 + 4*t^5.951 + 2*t^5.956 + t^5.991 + 2*t^5.995 + t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail