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
58903 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{3}$ 1.3149 1.5584 0.8438 [X:[], M:[1.1048], q:[0.5968, 0.4063], qb:[0.2984, 0.2984], phi:[0.4]] [X:[], M:[[-3]], q:[[2], [-4]], qb:[[1], [1]], phi:[[0]]] 1 {a: 386587/294000, c: 229081/147000, M1: 116/105, q1: 188/315, q2: 128/315, qb1: 94/315, qb2: 94/315, phi1: 2/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ 3}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ 2}\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ 6 2*t^2.11 + t^2.4 + t^2.69 + 3*t^3.31 + t^3.6 + 4*t^3.89 + 3*t^4.23 + 4*t^4.51 + 3*t^4.8 + 5*t^5.09 + t^5.37 + 6*t^5.43 + 5*t^5.71 + 6*t^6. + 9*t^6.29 + 4*t^6.34 + 2*t^6.57 + 13*t^6.63 + 8*t^6.91 + 16*t^7.2 + t^7.26 + 7*t^7.49 + 9*t^7.54 + 9*t^7.77 + 15*t^7.83 + t^8.06 + 9*t^8.11 + 24*t^8.4 + 5*t^8.46 + 6*t^8.69 + 20*t^8.74 + 15*t^8.97 - t^4.2/y - t^5.4/y - (2*t^6.31)/y - t^6.6/y - t^6.89/y + t^7.23/y - t^7.51/y + t^7.8/y + (3*t^8.43)/y - t^4.2*y - t^5.4*y - 2*t^6.31*y - t^6.6*y - t^6.89*y + t^7.23*y - t^7.51*y + t^7.8*y + 3*t^8.43*y (2*t^2.11)/g1^3 + t^2.4 + g1^3*t^2.69 + (3*t^3.31)/g1^3 + t^3.6 + 4*g1^3*t^3.89 + (3*t^4.23)/g1^6 + (4*t^4.51)/g1^3 + 3*t^4.8 + 5*g1^3*t^5.09 + g1^6*t^5.37 + (6*t^5.43)/g1^6 + (5*t^5.71)/g1^3 + 6*t^6. + 9*g1^3*t^6.29 + (4*t^6.34)/g1^9 + 2*g1^6*t^6.57 + (13*t^6.63)/g1^6 + (8*t^6.91)/g1^3 + 16*t^7.2 + t^7.26/g1^12 + 7*g1^3*t^7.49 + (9*t^7.54)/g1^9 + 9*g1^6*t^7.77 + (15*t^7.83)/g1^6 + g1^9*t^8.06 + (9*t^8.11)/g1^3 + 24*t^8.4 + (5*t^8.46)/g1^12 + 6*g1^3*t^8.69 + (20*t^8.74)/g1^9 + 15*g1^6*t^8.97 - t^4.2/y - t^5.4/y - (2*t^6.31)/(g1^3*y) - t^6.6/y - (g1^3*t^6.89)/y + t^7.23/(g1^6*y) - t^7.51/(g1^3*y) + t^7.8/y + (3*t^8.43)/(g1^6*y) - t^4.2*y - t^5.4*y - (2*t^6.31*y)/g1^3 - t^6.6*y - g1^3*t^6.89*y + (t^7.23*y)/g1^6 - (t^7.51*y)/g1^3 + t^7.8*y + (3*t^8.43*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
57441 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ 1.3154 1.5597 0.8434 [M:[1.0922], q:[0.597, 0.4059], qb:[0.3107, 0.2863], phi:[0.4]] t^2.077 + t^2.15 + t^2.4 + t^2.65 + 2*t^3.277 + t^3.35 + t^3.6 + 2*t^3.85 + 2*t^3.923 + t^4.153 + t^4.227 + t^4.3 + 2*t^4.477 + 2*t^4.55 + t^4.727 + 2*t^4.8 + 3*t^5.05 + 2*t^5.123 + t^5.3 + 2*t^5.353 + 3*t^5.427 + t^5.5 + 3*t^5.677 + 2*t^5.75 + 3*t^5.927 + 2*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail