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
58480 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ 1.2977 1.4612 0.8881 [X:[1.3846], M:[1.0769], q:[0.7949, 0.3333], qb:[0.4359, 0.5897], phi:[0.3077]] [X:[[0]], M:[[0]], q:[[-1], [-1]], qb:[[1], [1]], phi:[[0]]] 1 {a: 22809/17576, c: 12841/8788, X1: 18/13, M1: 14/13, q1: 31/39, q2: 1/3, qb1: 17/39, qb2: 23/39, phi1: 4/13}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}\phi_{1}^{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ 1 t^2.31 + t^2.77 + 2*t^3.23 + 2*t^3.69 + 3*t^4.15 + 2*t^4.62 + 2*t^5.08 + 2*t^5.31 + 2*t^5.54 + 2*t^5.77 + t^6. + 2*t^6.23 + 5*t^6.46 + 2*t^6.69 + 6*t^6.92 + 8*t^7.38 + 9*t^7.85 + 8*t^8.31 + 4*t^8.54 + 7*t^8.77 + t^8.77/y^2 - t^3.92/y - t^4.85/y - t^6.23/y - t^6.69/y - (2*t^7.15)/y - (2*t^7.62)/y - (2*t^8.08)/y - t^3.92*y - t^4.85*y - t^6.23*y - t^6.69*y - 2*t^7.15*y - 2*t^7.62*y - 2*t^8.08*y + t^8.77*y^2 t^2.31 + t^2.77 + 2*t^3.23 + 2*t^3.69 + 3*t^4.15 + 2*t^4.62 + 2*t^5.08 + t^5.31/g1^3 + g1^3*t^5.31 + 2*t^5.54 + t^5.77/g1^3 + g1^3*t^5.77 + t^6. + t^6.23/g1^3 + g1^3*t^6.23 + 5*t^6.46 + t^6.69/g1^3 + g1^3*t^6.69 + 6*t^6.92 + 8*t^7.38 + 9*t^7.85 + 8*t^8.31 + (2*t^8.54)/g1^3 + 2*g1^3*t^8.54 + 7*t^8.77 + t^8.77/y^2 - t^3.92/y - t^4.85/y - t^6.23/y - t^6.69/y - (2*t^7.15)/y - (2*t^7.62)/y - (2*t^8.08)/y - t^3.92*y - t^4.85*y - t^6.23*y - t^6.69*y - 2*t^7.15*y - 2*t^7.62*y - 2*t^8.08*y + t^8.77*y^2


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
57378 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ 1.3384 1.4989 0.8929 [X:[1.4315], M:[0.8423], q:[0.7088, 0.435], qb:[0.4281, 0.7227], phi:[0.2842]] t^2.527 + t^2.558 + t^2.589 + t^3.411 + t^3.442 + t^4.263 + 3*t^4.295 + t^4.326 + t^5.054 + t^5.085 + 2*t^5.116 + 2*t^5.147 + t^5.179 + 2*t^5.589 + t^5.938 + t^5.969 - t^6. - t^3.853/y - t^4.705/y - t^3.853*y - t^4.705*y detail