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
59439 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ 1.1873 1.4179 0.8374 [X:[1.5106], M:[0.8], q:[0.6071, 0.3859], qb:[0.5035, 0.1035], phi:[0.4]] [X:[[3]], M:[[0]], q:[[2], [-4]], qb:[[1], [1]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{3}$ 2 t^2.13 + 2*t^2.4 + 2*t^2.67 + 3*t^3.33 + 2*t^3.87 + t^4.26 + 8*t^4.53 + 4*t^4.8 + 5*t^5.07 + 3*t^5.34 + 3*t^5.46 + 9*t^5.73 + 2*t^6. + 3*t^6.27 + t^6.4 + 4*t^6.54 + 11*t^6.66 + 14*t^6.93 + t^7.07 + 15*t^7.2 + 6*t^7.47 + 3*t^7.6 + 11*t^7.74 + 21*t^7.86 + 3*t^8. + 9*t^8.13 + 14*t^8.4 + t^8.53 - t^8.67 + 11*t^8.8 + 7*t^8.94 - t^4.2/y - t^5.4/y - t^6.33/y - (2*t^6.6)/y - t^6.87/y + (2*t^7.8)/y + (2*t^8.07)/y + t^8.34/y + (2*t^8.46)/y + t^8.73/y - t^4.2*y - t^5.4*y - t^6.33*y - 2*t^6.6*y - t^6.87*y + 2*t^7.8*y + 2*t^8.07*y + t^8.34*y + 2*t^8.46*y + t^8.73*y g1^3*t^2.13 + 2*t^2.4 + (2*t^2.67)/g1^3 + 3*g1^3*t^3.33 + (2*t^3.87)/g1^3 + g1^6*t^4.26 + 8*g1^3*t^4.53 + 4*t^4.8 + (5*t^5.07)/g1^3 + (3*t^5.34)/g1^6 + 3*g1^6*t^5.46 + 9*g1^3*t^5.73 + 2*t^6. + (3*t^6.27)/g1^3 + g1^9*t^6.4 + (4*t^6.54)/g1^6 + 11*g1^6*t^6.66 + 14*g1^3*t^6.93 + t^7.07/g1^12 + 15*t^7.2 + (6*t^7.47)/g1^3 + 3*g1^9*t^7.6 + (11*t^7.74)/g1^6 + 21*g1^6*t^7.86 + (3*t^8.)/g1^9 + 9*g1^3*t^8.13 + 14*t^8.4 + g1^12*t^8.53 - t^8.67/g1^3 + 11*g1^9*t^8.8 + (7*t^8.94)/g1^6 - t^4.2/y - t^5.4/y - (g1^3*t^6.33)/y - (2*t^6.6)/y - t^6.87/(g1^3*y) + (2*t^7.8)/y + (2*t^8.07)/(g1^3*y) + t^8.34/(g1^6*y) + (2*g1^6*t^8.46)/y + (g1^3*t^8.73)/y - t^4.2*y - t^5.4*y - g1^3*t^6.33*y - 2*t^6.6*y - (t^6.87*y)/g1^3 + 2*t^7.8*y + (2*t^8.07*y)/g1^3 + (t^8.34*y)/g1^6 + 2*g1^6*t^8.46*y + g1^3*t^8.73*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
57596 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ 1.1708 1.3889 0.843 [X:[1.5106], M:[], q:[0.6071, 0.3859], qb:[0.5035, 0.1035], phi:[0.4]] t^2.13 + t^2.4 + 2*t^2.67 + 3*t^3.33 + t^3.6 + 2*t^3.87 + t^4.26 + 7*t^4.53 + 2*t^4.8 + 3*t^5.07 + 3*t^5.34 + 3*t^5.46 + 7*t^5.73 + 3*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail