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
58406 SU3adj1nf2 ${}\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ 1.0942 1.2349 0.8861 [X:[1.5], M:[0.75], q:[0.4167, 0.6667], qb:[1.0833, 0.3333], phi:[0.25]] [X:[[0]], M:[[0]], q:[[-1], [-1]], qb:[[1], [1]], phi:[[0]]] 1 {a: 2241/2048, c: 2529/2048, X1: 3/2, M1: 3/4, q1: 5/12, q2: 2/3, qb1: 13/12, qb2: 1/3, phi1: 1/4}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{6}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ ${}\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ 2 3*t^2.25 + 2*t^3. + 8*t^4.5 + 8*t^5.25 + 2*t^6. + 13*t^6.75 + 18*t^7.5 + 5*t^8.25 + t^8.25/y^2 - t^3.75/y - t^4.5/y - (3*t^6.)/y - (4*t^6.75)/y + (3*t^7.5)/y - t^3.75*y - t^4.5*y - 3*t^6.*y - 4*t^6.75*y + 3*t^7.5*y + t^8.25*y^2 3*t^2.25 + 2*t^3. + 8*t^4.5 + 6*t^5.25 + t^5.25/g1^3 + g1^3*t^5.25 + t^6./g1^3 + g1^3*t^6. + 13*t^6.75 + 14*t^7.5 + (2*t^7.5)/g1^3 + 2*g1^3*t^7.5 - t^8.25 + (3*t^8.25)/g1^3 + 3*g1^3*t^8.25 + t^8.25/y^2 - t^3.75/y - t^4.5/y - (3*t^6.)/y - (4*t^6.75)/y + (3*t^7.5)/y - t^3.75*y - t^4.5*y - 3*t^6.*y - 4*t^6.75*y + 3*t^7.5*y + t^8.25*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
57359 SU3adj1nf2 ${}\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ 1.3052 1.4458 0.9027 [X:[1.5], M:[0.75], q:[0.75, 0.5], qb:[0.75, 0.5], phi:[0.25]] 2*t^2.25 + t^3. + 2*t^3.75 + 8*t^4.5 + 3*t^5.25 + 2*t^6. - t^3.75/y - t^4.5/y - (2*t^6.)/y - t^3.75*y - t^4.5*y - 2*t^6.*y detail {a: 2673/2048, c: 2961/2048, X1: 3/2, M1: 3/4, q1: 3/4, q2: 1/2, qb1: 3/4, qb2: 1/2, phi1: 1/4}