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
61144 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ + ${ }q_{2}\tilde{q}_{1}X_{1}$ 1.1451 1.3588 0.8427 [X:[1.6], M:[0.7804, 1.2], q:[0.6798, 0.2601], qb:[0.1399, 0.5202], phi:[0.4]] [X:[[0]], M:[[3], [0]], q:[[-2], [1]], qb:[[-1], [2]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ ${}M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ 2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}^{3}\tilde{q}_{2}$ 3 2*t^2.34 + t^2.4 + t^2.46 + t^3.54 + 5*t^3.6 + 3*t^4.68 + 3*t^4.74 + 7*t^4.8 + 2*t^4.86 + t^4.92 + 2*t^5.88 + 11*t^5.94 + 3*t^6. + 5*t^6.06 + 4*t^7.02 + 6*t^7.08 + 14*t^7.14 + 16*t^7.2 + 3*t^7.26 + 2*t^7.32 + t^7.38 + 3*t^8.22 + 18*t^8.28 + 9*t^8.34 + 18*t^8.4 + t^8.46 + 5*t^8.52 - t^4.2/y - t^5.4/y - (2*t^6.54)/y - t^6.66/y + t^7.68/y - t^7.8/y + t^7.86/y - t^8.88/y + (11*t^8.94)/y - t^4.2*y - t^5.4*y - 2*t^6.54*y - t^6.66*y + t^7.68*y - t^7.8*y + t^7.86*y - t^8.88*y + 11*t^8.94*y 2*g1^3*t^2.34 + t^2.4 + t^2.46/g1^3 + g1^3*t^3.54 + 5*t^3.6 + 3*g1^6*t^4.68 + 3*g1^3*t^4.74 + 7*t^4.8 + (2*t^4.86)/g1^3 + t^4.92/g1^6 + 2*g1^6*t^5.88 + 11*g1^3*t^5.94 + 3*t^6. + (5*t^6.06)/g1^3 + 4*g1^9*t^7.02 + 6*g1^6*t^7.08 + 14*g1^3*t^7.14 + 16*t^7.2 + (3*t^7.26)/g1^3 + (2*t^7.32)/g1^6 + t^7.38/g1^9 + 3*g1^9*t^8.22 + 18*g1^6*t^8.28 + 9*g1^3*t^8.34 + 18*t^8.4 + t^8.46/g1^3 + (5*t^8.52)/g1^6 - t^4.2/y - t^5.4/y - (2*g1^3*t^6.54)/y - t^6.66/(g1^3*y) + (g1^6*t^7.68)/y - t^7.8/y + t^7.86/(g1^3*y) - (g1^6*t^8.88)/y + (11*g1^3*t^8.94)/y - t^4.2*y - t^5.4*y - 2*g1^3*t^6.54*y - (t^6.66*y)/g1^3 + g1^6*t^7.68*y - t^7.8*y + (t^7.86*y)/g1^3 - g1^6*t^8.88*y + 11*g1^3*t^8.94*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
58451 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ 1.4105 1.6615 0.8489 [X:[], M:[0.7838, 1.2], q:[0.4098, 0.3951], qb:[0.4065, 0.3887], 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 + 4*t^4.75 + 2*t^4.76 + t^4.79 + 7*t^4.8 + t^4.81 + 2*t^4.84 + 2*t^4.85 + t^4.9 + 2*t^5.9 + 7*t^5.95 + 2*t^5.96 + t^5.99 + 5*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail