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
58392 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{5}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{2}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ 1.1671 1.3796 0.846 [X:[1.5145, 1.2855], M:[0.8], q:[0.3806, 0.6097], qb:[0.5048, 0.1048], phi:[0.4]] [X:[[-3], [3]], M:[[0]], q:[[4], [-2]], qb:[[-1], [-1]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ 0 2*t^2.4 + 2*t^2.66 + 3*t^3.34 + 3*t^3.86 + 6*t^4.54 + 2*t^4.8 + 5*t^5.06 + 3*t^5.31 + 9*t^5.74 + 5*t^6.26 + 6*t^6.51 + 3*t^6.69 + 10*t^6.94 + t^7.03 + 13*t^7.2 + 3*t^7.46 + 14*t^7.71 + 12*t^7.89 + 3*t^7.97 + 7*t^8.14 + 17*t^8.4 - 3*t^8.66 + 12*t^8.91 - t^4.2/y - t^5.4/y - (2*t^6.6)/y - t^6.86/y - t^7.54/y + t^8.06/y + t^8.31/y + (3*t^8.74)/y - t^4.2*y - t^5.4*y - 2*t^6.6*y - t^6.86*y - t^7.54*y + t^8.06*y + t^8.31*y + 3*t^8.74*y 2*t^2.4 + 2*g1^3*t^2.66 + (3*t^3.34)/g1^3 + 3*g1^3*t^3.86 + (6*t^4.54)/g1^3 + 2*t^4.8 + 5*g1^3*t^5.06 + 3*g1^6*t^5.31 + (9*t^5.74)/g1^3 + 5*g1^3*t^6.26 + 6*g1^6*t^6.51 + (3*t^6.69)/g1^6 + (10*t^6.94)/g1^3 + g1^12*t^7.03 + 13*t^7.2 + 3*g1^3*t^7.46 + 14*g1^6*t^7.71 + (12*t^7.89)/g1^6 + 3*g1^9*t^7.97 + (7*t^8.14)/g1^3 + 17*t^8.4 - 3*g1^3*t^8.66 + 12*g1^6*t^8.91 - t^4.2/y - t^5.4/y - (2*t^6.6)/y - (g1^3*t^6.86)/y - t^7.54/(g1^3*y) + (g1^3*t^8.06)/y + (g1^6*t^8.31)/y + (3*t^8.74)/(g1^3*y) - t^4.2*y - t^5.4*y - 2*t^6.6*y - g1^3*t^6.86*y - (t^7.54*y)/g1^3 + g1^3*t^8.06*y + g1^6*t^8.31*y + (3*t^8.74*y)/g1^3


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
60944 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{5}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{2}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ 1.1779 1.3984 0.8423 [X:[1.5279, 1.2721], M:[0.8, 0.8721], q:[0.3627, 0.6186], qb:[0.5093, 0.1093], phi:[0.4]] 2*t^2.4 + 3*t^2.62 + 2*t^3.38 + 3*t^3.82 + 6*t^4.58 + 2*t^4.8 + 7*t^5.02 + 6*t^5.23 + 7*t^5.78 - 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
57343 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{5}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{2}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ 1.1506 1.3506 0.8519 [X:[1.5145, 1.2855], q:[0.3806, 0.6097], qb:[0.5048, 0.1048], phi:[0.4]] t^2.4 + 2*t^2.656 + 3*t^3.344 + t^3.6 + 3*t^3.856 + 6*t^4.544 + 3*t^5.056 + 3*t^5.313 + 6*t^5.744 + t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail