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
1271 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{6}q_{2}\tilde{q}_{2}$ 0.7284 0.9028 0.8068 [M:[0.9169, 0.9169, 1.0831, 0.7506, 0.9169, 0.9169], q:[0.6247, 0.4584], qb:[0.4584, 0.6247], phi:[0.4584]] [M:[[-2], [-2], [2], [-6], [-2], [-2]], q:[[3], [-1]], qb:[[-1], [3]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{1}$, ${ }M_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ ${}M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ -3 t^2.252 + 5*t^2.751 + t^3.249 + 3*t^4.126 + t^4.503 + 4*t^4.625 + 5*t^5.002 + 3*t^5.124 + 12*t^5.501 - 3*t^6. + 3*t^6.378 - 4*t^6.499 + t^6.755 + 15*t^6.876 + 5*t^7.254 + 12*t^7.375 + 12*t^7.753 + 4*t^7.874 + 20*t^8.252 - 4*t^8.373 + 3*t^8.629 - 18*t^8.751 - t^4.375/y - t^6.627/y - (4*t^7.126)/y + (4*t^7.625)/y + (5*t^8.002)/y + t^8.124/y + (11*t^8.501)/y - t^8.879/y - t^4.375*y - t^6.627*y - 4*t^7.126*y + 4*t^7.625*y + 5*t^8.002*y + t^8.124*y + 11*t^8.501*y - t^8.879*y t^2.252/g1^6 + (5*t^2.751)/g1^2 + g1^2*t^3.249 + (3*t^4.126)/g1^3 + t^4.503/g1^12 + 4*g1*t^4.625 + (5*t^5.002)/g1^8 + 3*g1^5*t^5.124 + (12*t^5.501)/g1^4 - 3*t^6. + (3*t^6.378)/g1^9 - 4*g1^4*t^6.499 + t^6.755/g1^18 + (15*t^6.876)/g1^5 + (5*t^7.254)/g1^14 + (12*t^7.375)/g1 + (12*t^7.753)/g1^10 + 4*g1^3*t^7.874 + (20*t^8.252)/g1^6 - 4*g1^7*t^8.373 + (3*t^8.629)/g1^15 - (18*t^8.751)/g1^2 - t^4.375/(g1*y) - t^6.627/(g1^7*y) - (4*t^7.126)/(g1^3*y) + (4*g1*t^7.625)/y + (5*t^8.002)/(g1^8*y) + (g1^5*t^8.124)/y + (11*t^8.501)/(g1^4*y) - t^8.879/(g1^13*y) - (t^4.375*y)/g1 - (t^6.627*y)/g1^7 - (4*t^7.126*y)/g1^3 + 4*g1*t^7.625*y + (5*t^8.002*y)/g1^8 + g1^5*t^8.124*y + (11*t^8.501*y)/g1^4 - (t^8.879*y)/g1^13


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
793 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ 0.7211 0.8891 0.811 [M:[0.9247, 0.9247, 1.0753, 0.774, 0.9247], q:[0.613, 0.4623], qb:[0.4623, 0.613], phi:[0.4623]] t^2.322 + 4*t^2.774 + 2*t^3.226 + 3*t^4.161 + 4*t^4.613 + t^4.644 + 3*t^5.065 + 4*t^5.096 + 8*t^5.548 - t^4.387/y - t^4.387*y detail