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
45787 SU3adj1nf1 ${}\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}X_{2}$ + ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }M_{1}^{2}$ 0.909 0.984 0.9238 [X:[1.6, 1.4], M:[1.0, 0.8], q:[0.3333], qb:[0.4667], phi:[0.2]] [X:[[0], [0]], M:[[0], [0]], q:[[0]], qb:[[0]], phi:[[0]]] 0 {a: 909/1000, c: 123/125, X1: 8/5, X2: 7/5, M1: 1, M2: 4/5, q1: 1/3, qb1: 7/15, phi1: 1/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }X_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }X_{1}$, ${ }M_{1}M_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$ ${}$ 0 2*t^2.4 + t^3. + t^4.2 + 5*t^4.8 + 2*t^5.4 + t^6.6 + 8*t^7.2 + 4*t^7.8 - t^8.4 + t^7.8/y^2 - t^3.6/y - t^4.2/y - (2*t^6.)/y - (2*t^6.6)/y + t^7.8/y - (2*t^8.4)/y - t^3.6*y - t^4.2*y - 2*t^6.*y - 2*t^6.6*y + t^7.8*y - 2*t^8.4*y + t^7.8*y^2 2*t^2.4 + t^3. + t^4.2 + 5*t^4.8 + 2*t^5.4 + t^6.6 + 8*t^7.2 + 4*t^7.8 - t^8.4 + t^7.8/y^2 - t^3.6/y - t^4.2/y - (2*t^6.)/y - (2*t^6.6)/y + t^7.8/y - (2*t^8.4)/y - t^3.6*y - t^4.2*y - 2*t^6.*y - 2*t^6.6*y + t^7.8*y - 2*t^8.4*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


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
61066 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}X_{2}$ + ${ }M_{1}\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$ 0.909 0.984 0.9238 [X:[1.6, 1.4], M:[0.8], q:[0.7333, 0.3333], qb:[0.4667, 1.2667], phi:[0.2]] 2*t^2.4 + t^3. + t^4.2 + 5*t^4.8 + 2*t^5.4 - t^3.6/y - t^4.2/y - (2*t^6.)/y - t^3.6*y - t^4.2*y - 2*t^6.*y detail {a: 909/1000, c: 123/125, X1: 8/5, X2: 7/5, M1: 4/5, q1: 11/15, q2: 1/3, qb1: 7/15, qb2: 19/15, phi1: 1/5}


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
45776 SU3adj1nf1 ${}\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}X_{2}$ + ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}q_{1}\tilde{q}_{1}$ 0.9394 1.0045 0.9352 [X:[1.653, 1.4795], M:[0.8675, 0.694], q:[0.4658], qb:[0.4932], phi:[0.1735]] t^2.08 + t^2.6 + t^2.88 + t^4.16 + t^4.44 + t^4.68 + 2*t^4.96 + t^5.21 + t^5.48 + 2*t^5.75 - t^6. - t^3.52/y - t^4.04/y - t^5.6/y - t^3.52*y - t^4.04*y - t^5.6*y detail