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
57500 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}X_{2}$ 0.9904 1.0529 0.9406 [X:[1.6, 1.4], M:[], q:[0.5667, 0.5667], qb:[0.4333, 1.2333], phi:[0.2]] [X:[[0], [0]], M:[], q:[[-1], [-1]], qb:[[1], [1]], phi:[[0]]] 1 {a: 7923/8000, c: 8423/8000, X1: 8/5, X2: 7/5, q1: 17/30, q2: 17/30, qb1: 13/30, qb2: 37/30, phi1: 1/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }X_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$ ${}$ -1 2*t^3. + t^3.6 + 2*t^4.2 + 2*t^5.4 + 2*t^5.7 - t^6. + t^6.6 + 2*t^6.9 + 3*t^7.2 - 2*t^7.5 + 5*t^7.8 - 2*t^8.1 + 5*t^8.4 + t^7.8/y^2 - t^3.6/y - t^4.2/y - (2*t^6.6)/y - t^7.2/y - (2*t^7.8)/y - t^3.6*y - t^4.2*y - 2*t^6.6*y - t^7.2*y - 2*t^7.8*y + t^7.8*y^2 2*t^3. + t^3.6 + 2*t^4.2 + 2*t^5.4 + t^5.7/g1^3 + g1^3*t^5.7 - t^6. + t^6.6 + t^6.9/g1^3 + g1^3*t^6.9 + 3*t^7.2 - t^7.5/g1^3 - g1^3*t^7.5 + 5*t^7.8 - t^8.1/g1^3 - g1^3*t^8.1 + 5*t^8.4 + t^7.8/y^2 - t^3.6/y - t^4.2/y - (2*t^6.6)/y - t^7.2/y - (2*t^7.8)/y - t^3.6*y - t^4.2*y - 2*t^6.6*y - t^7.2*y - 2*t^7.8*y + t^7.8*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
59441 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}X_{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ 1.0069 1.0819 0.9307 [X:[1.6, 1.4], M:[0.8], q:[0.5667, 0.5667], qb:[0.4333, 1.2333], phi:[0.2]] t^2.4 + 2*t^3. + 2*t^4.2 + t^4.8 + 4*t^5.4 + 2*t^5.7 - t^6. - t^3.6/y - t^4.2/y - t^6./y - t^3.6*y - t^4.2*y - t^6.*y detail {a: 1611/1600, c: 1731/1600, X1: 8/5, X2: 7/5, M1: 4/5, q1: 17/30, q2: 17/30, qb1: 13/30, qb2: 37/30, phi1: 1/5}


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
47910 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ 1.1092 1.231 0.9011 [X:[1.5086], q:[0.8484, 0.3915], qb:[0.38, 0.9059], phi:[0.2457]] t^2.211 + t^2.315 + t^3.052 + t^3.685 + t^3.789 + t^3.892 + t^4.422 + 2*t^4.526 + t^4.629 + 2*t^5.263 + t^5.367 + 2*t^5.631 + 2*t^5.735 - t^6. - t^3.737/y - t^4.474/y - t^5.948/y - t^3.737*y - t^4.474*y - t^5.948*y detail