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
59418 SU3adj1nf2 ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}^{2}$ 0.953 1.1458 0.8317 [X:[1.585, 1.415, 1.585, 1.415], M:[0.915], q:[0.1383, 0.3084], qb:[0.2766, 0.2766], phi:[0.5]] [X:[[-3], [3], [-3], [3]], M:[[3]], q:[[1], [-5]], qb:[[2], [2]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{2}$, ${ }X_{4}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }X_{3}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{3}$ ${}M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{2}^{2}$ 0 3*t^2.74 + t^3. + 2*t^3.26 + t^3.77 + 2*t^3.99 + 4*t^4.24 + t^4.5 + 5*t^4.76 + t^5.27 + 7*t^5.49 + 2*t^5.74 + t^6.51 + 4*t^6.73 + t^6.77 + 15*t^6.99 + 2*t^7.02 + 4*t^7.24 + t^7.28 + 14*t^7.5 + t^7.53 + 3*t^7.76 + 3*t^7.98 + 8*t^8.01 + 13*t^8.23 + 9*t^8.49 + 3*t^8.52 - 6*t^8.74 - t^8.78 - t^4.5/y - t^6./y - t^7.24/y + t^7.5/y + t^7.76/y + (3*t^8.49)/y - (2*t^8.74)/y - t^4.5*y - t^6.*y - t^7.24*y + t^7.5*y + t^7.76*y + 3*t^8.49*y - 2*t^8.74*y 3*g1^3*t^2.74 + t^3. + (2*t^3.26)/g1^3 + t^3.77/g1^9 + 2*g1^6*t^3.99 + 4*g1^3*t^4.24 + t^4.5 + (5*t^4.76)/g1^3 + t^5.27/g1^9 + 7*g1^6*t^5.49 + 2*g1^3*t^5.74 + t^6.51/g1^6 + 4*g1^9*t^6.73 + t^6.77/g1^9 + 15*g1^6*t^6.99 + (2*t^7.02)/g1^12 + 4*g1^3*t^7.24 + t^7.28/g1^15 + 14*t^7.5 + t^7.53/g1^18 + (3*t^7.76)/g1^3 + 3*g1^12*t^7.98 + (8*t^8.01)/g1^6 + 13*g1^9*t^8.23 + 9*g1^6*t^8.49 + (3*t^8.52)/g1^12 - 6*g1^3*t^8.74 - t^8.78/g1^15 - t^4.5/y - t^6./y - (g1^3*t^7.24)/y + t^7.5/y + t^7.76/(g1^3*y) + (3*g1^6*t^8.49)/y - (2*g1^3*t^8.74)/y - t^4.5*y - t^6.*y - g1^3*t^7.24*y + t^7.5*y + (t^7.76*y)/g1^3 + 3*g1^6*t^8.49*y - 2*g1^3*t^8.74*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
57683 SU3adj1nf2 ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ 0.9587 1.1535 0.8311 [X:[1.6173, 1.4795, 1.5205, 1.3827], M:[0.8827], q:[0.1598, 0.2976], qb:[0.2228, 0.3197], phi:[0.5]] 2*t^2.65 + t^2.94 + t^3. + t^3.06 + t^3.35 + t^3.77 + t^3.8 + t^4.09 + 2*t^4.15 + 2*t^4.44 + t^4.5 + 2*t^4.56 + 3*t^4.85 + t^5.27 + 4*t^5.3 + 2*t^5.59 + t^5.65 + t^5.71 + t^5.88 + t^5.94 - t^6. - t^4.5/y - t^6./y - t^4.5*y - t^6.*y detail