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
57802 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{6}$ 1.4747 1.6831 0.8762 [X:[1.3333], M:[0.9833, 0.6833], q:[0.4835, 0.5168], qb:[0.4999, 0.4999], phi:[0.3333]] [X:[[0, 0]], M:[[-1, -1], [1, 1]], q:[[-1, -2], [1, 0]], qb:[[0, 1], [0, 1]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ ${}M_{2}\phi_{1}q_{1}\tilde{q}_{2}$ -1 t^2.05 + 3*t^2.95 + t^3. + t^3.05 + t^3.95 + t^4. + 2*t^4.05 + t^4.1 + 2*t^4.95 + 3*t^5. + 3*t^5.05 + t^5.1 + t^5.45 + 2*t^5.5 + t^5.55 + 5*t^5.9 + 3*t^5.95 - t^6. + 2*t^6.05 + 2*t^6.1 + t^6.15 + t^6.45 + 2*t^6.5 + t^6.55 + 2*t^6.9 + 4*t^6.95 + 5*t^7. + 6*t^7.05 + 4*t^7.1 + t^7.15 + t^7.35 + 3*t^7.5 + 2*t^7.55 + t^7.6 + t^7.65 + 6*t^7.9 + 6*t^7.95 + 9*t^8. + t^8.05 + 6*t^8.1 + 2*t^8.15 + t^8.2 + t^8.4 + 3*t^8.45 + 3*t^8.5 + t^8.55 + 7*t^8.85 + 7*t^8.9 - 6*t^8.95 - t^4./y - t^5./y - t^6.05/y - (3*t^6.95)/y - t^7./y - (2*t^7.05)/y - (2*t^7.95)/y + (2*t^8.)/y + (3*t^8.9)/y + (2*t^8.95)/y - t^4.*y - t^5.*y - t^6.05*y - 3*t^6.95*y - t^7.*y - 2*t^7.05*y - 2*t^7.95*y + 2*t^8.*y + 3*t^8.9*y + 2*t^8.95*y g1*g2*t^2.05 + (3*t^2.95)/(g1*g2) + t^3. + g1*g2*t^3.05 + t^3.95/(g1*g2) + t^4. + 2*g1*g2*t^4.05 + g1^2*g2^2*t^4.1 + (2*t^4.95)/(g1*g2) + 3*t^5. + 3*g1*g2*t^5.05 + g1^2*g2^2*t^5.1 + t^5.45/(g1*g2^4) + 2*g2^3*t^5.5 + (g1*t^5.55)/g2^2 + (5*t^5.9)/(g1^2*g2^2) + (3*t^5.95)/(g1*g2) - t^6. + 2*g1*g2*t^6.05 + 2*g1^2*g2^2*t^6.1 + g1^3*g2^3*t^6.15 + t^6.45/(g1*g2^4) + 2*g2^3*t^6.5 + (g1*t^6.55)/g2^2 + (2*t^6.9)/(g1^2*g2^2) + (4*t^6.95)/(g1*g2) + 5*t^7. + 6*g1*g2*t^7.05 + 4*g1^2*g2^2*t^7.1 + g1^3*g2^3*t^7.15 + t^7.35/(g1^3*g2^6) + t^7.45/(g1*g2^4) - (g2^2*t^7.45)/g1 - t^7.5/g2^3 + 4*g2^3*t^7.5 + (g1*t^7.55)/g2^2 + g1*g2^4*t^7.55 + (g1^2*t^7.6)/g2 + g1^3*t^7.65 + (6*t^7.9)/(g1^2*g2^2) + (6*t^7.95)/(g1*g2) + 9*t^8. + g1*g2*t^8.05 + 6*g1^2*g2^2*t^8.1 + 2*g1^3*g2^3*t^8.15 + g1^4*g2^4*t^8.2 + t^8.4/(g1^2*g2^5) + t^8.45/(g1*g2^4) + (2*g2^2*t^8.45)/g1 + t^8.5/g2^3 + 2*g2^3*t^8.5 + (g1*t^8.55)/g2^2 + (7*t^8.85)/(g1^3*g2^3) + (7*t^8.9)/(g1^2*g2^2) - (6*t^8.95)/(g1*g2) - t^4./y - t^5./y - (g1*g2*t^6.05)/y - (3*t^6.95)/(g1*g2*y) - t^7./y - (2*g1*g2*t^7.05)/y - (2*t^7.95)/(g1*g2*y) + (2*t^8.)/y + (3*t^8.9)/(g1^2*g2^2*y) + (2*t^8.95)/(g1*g2*y) - t^4.*y - t^5.*y - g1*g2*t^6.05*y - (3*t^6.95*y)/(g1*g2) - t^7.*y - 2*g1*g2*t^7.05*y - (2*t^7.95*y)/(g1*g2) + 2*t^8.*y + (3*t^8.9*y)/(g1^2*g2^2) + (2*t^8.95*y)/(g1*g2)


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
57286 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$ 1.4759 1.6818 0.8775 [X:[1.3442], M:[0.9514, 0.6882], q:[0.4921, 0.5242], qb:[0.4919, 0.5244], phi:[0.3279]] t^2.064 + t^2.854 + t^2.951 + t^2.952 + t^3.048 + t^3.049 + t^4.032 + 2*t^4.033 + t^4.129 + t^4.13 + 2*t^4.919 + 3*t^5.016 + t^5.017 + 2*t^5.113 + t^5.114 + t^5.508 + t^5.509 + t^5.605 + t^5.606 + t^5.708 + t^5.805 + t^5.806 + t^5.902 + t^5.903 + t^5.904 + t^5.999 - 3*t^6. - t^3.984/y - t^4.967/y - t^3.984*y - t^4.967*y detail