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
47911 SU3adj1nf2 ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{6}$ 1.4406 1.6281 0.8848 [X:[1.3333], q:[0.5771, 0.5124], qb:[0.4552, 0.4552], phi:[0.3333]] [X:[[0, 0]], q:[[1, 1], [-2, -2]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ ${}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ 2}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ 0 2*t^2.903 + t^3. + 2*t^3.097 + 2*t^3.903 + t^4. + 2*t^4.097 + 2*t^4.903 + 4*t^5.097 + 3*t^5.806 + 2*t^5.903 + 4*t^6.097 + 2*t^6.194 + 4*t^6.806 + 4*t^6.903 + 4*t^7. + 8*t^7.097 + 2*t^7.194 + t^7.611 + 7*t^7.806 + 9*t^8. + 4*t^8.097 + 7*t^8.194 + 2*t^8.708 + 7*t^8.806 - 4*t^8.903 - t^4./y - t^5./y - (2*t^6.903)/y - t^7./y - (2*t^7.097)/y - (2*t^7.903)/y - t^8./y - (2*t^8.097)/y + t^8.806/y - t^4.*y - t^5.*y - 2*t^6.903*y - t^7.*y - 2*t^7.097*y - 2*t^7.903*y - t^8.*y - 2*t^8.097*y + t^8.806*y t^2.903/(g1*g2^2) + t^2.903/(g1^2*g2) + t^3. + g1^2*g2*t^3.097 + g1*g2^2*t^3.097 + t^3.903/(g1*g2^2) + t^3.903/(g1^2*g2) + t^4. + g1^2*g2*t^4.097 + g1*g2^2*t^4.097 + t^4.903/(g1*g2^2) + t^4.903/(g1^2*g2) + 2*g1^2*g2*t^5.097 + 2*g1*g2^2*t^5.097 + t^5.806/(g1^2*g2^4) + t^5.806/(g1^3*g2^3) + t^5.806/(g1^4*g2^2) + t^5.903/(g1*g2^2) + t^5.903/(g1^2*g2) + 2*g1^2*g2*t^6.097 + 2*g1*g2^2*t^6.097 + g1^4*g2^2*t^6.194 + g1^2*g2^4*t^6.194 + t^6.806/(g1^2*g2^4) + (2*t^6.806)/(g1^3*g2^3) + t^6.806/(g1^4*g2^2) + (2*t^6.903)/(g1*g2^2) + (2*t^6.903)/(g1^2*g2) + 2*t^7. + (g1*t^7.)/g2 + (g2*t^7.)/g1 + g1^3*t^7.097 + 3*g1^2*g2*t^7.097 + 3*g1*g2^2*t^7.097 + g2^3*t^7.097 + g1^4*g2^2*t^7.194 + g1^2*g2^4*t^7.194 + t^7.611/(g1^6*g2^6) + (2*t^7.806)/(g1^2*g2^4) + (3*t^7.806)/(g1^3*g2^3) + (2*t^7.806)/(g1^4*g2^2) + 5*t^8. + (2*g1*t^8.)/g2 + (2*g2*t^8.)/g1 + 2*g1^2*g2*t^8.097 + 2*g1*g2^2*t^8.097 + 2*g1^4*g2^2*t^8.194 + 3*g1^3*g2^3*t^8.194 + 2*g1^2*g2^4*t^8.194 + t^8.708/(g1^3*g2^6) + t^8.708/(g1^6*g2^3) + (2*t^8.806)/(g1^2*g2^4) + (3*t^8.806)/(g1^3*g2^3) + (2*t^8.806)/(g1^4*g2^2) - (2*t^8.903)/(g1*g2^2) - (2*t^8.903)/(g1^2*g2) - t^4./y - t^5./y - t^6.903/(g1*g2^2*y) - t^6.903/(g1^2*g2*y) - t^7./y - (g1^2*g2*t^7.097)/y - (g1*g2^2*t^7.097)/y - t^7.903/(g1*g2^2*y) - t^7.903/(g1^2*g2*y) - t^8./y - (g1^2*g2*t^8.097)/y - (g1*g2^2*t^8.097)/y + t^8.806/(g1^3*g2^3*y) - t^4.*y - t^5.*y - (t^6.903*y)/(g1*g2^2) - (t^6.903*y)/(g1^2*g2) - t^7.*y - g1^2*g2*t^7.097*y - g1*g2^2*t^7.097*y - (t^7.903*y)/(g1*g2^2) - (t^7.903*y)/(g1^2*g2) - t^8.*y - g1^2*g2*t^8.097*y - g1*g2^2*t^8.097*y + (t^8.806*y)/(g1^3*g2^3)


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
57507 ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{6}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ 1.4612 1.6678 0.8761 [X:[1.3333], M:[0.6939], q:[0.5755, 0.5157], qb:[0.4571, 0.4518], phi:[0.3333]] t^2.08 + t^2.9 + t^2.92 + t^3. + t^3.08 + t^3.1 + t^3.9 + t^4. + t^4.08 + t^4.1 + t^4.16 + t^4.9 + t^4.92 + t^4.98 + t^5. + 3*t^5.08 + 2*t^5.1 + t^5.16 + t^5.18 + t^5.8 + t^5.82 + t^5.84 + t^5.9 + t^5.92 + t^5.98 - t^4./y - t^5./y - t^4.*y - t^5.*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
47876 SU3adj1nf2 ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ 1.4426 1.6227 0.889 [X:[1.353], q:[0.5758, 0.525], qb:[0.4792, 0.4792], phi:[0.3235]] t^2.911 + 2*t^3.013 + 2*t^3.165 + 2*t^3.983 + t^4.059 + 2*t^4.135 + 2*t^4.953 + 2*t^5.106 + 2*t^5.283 + t^5.823 + 2*t^5.924 - 5*t^6. - t^3.97/y - t^4.941/y - t^3.97*y - t^4.941*y detail