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
55540 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{6}$ 0.6742 0.8533 0.7901 [M:[0.8665, 0.7834, 1.2166, 0.8665, 0.7834, 0.7834], q:[0.7003, 0.4332], qb:[0.7834, 0.3502], phi:[0.4332]] [M:[[-4], [1], [-1], [-4], [1], [1]], q:[[6], [-2]], qb:[[1], [3]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$ ${}M_{1}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ -1 3*t^2.35 + 3*t^2.599 + t^3.151 + t^3.401 + t^3.899 + 2*t^4.451 + 7*t^4.7 + 8*t^4.95 + 5*t^5.199 + 4*t^5.502 + 5*t^5.751 - t^6. - t^6.249 + t^6.303 + 2*t^6.498 + t^6.552 + 3*t^6.801 + 13*t^7.05 + 13*t^7.3 + 11*t^7.549 + 2*t^7.602 + 9*t^7.798 + 9*t^7.852 + 9*t^8.101 - 4*t^8.35 - 9*t^8.599 + 4*t^8.653 - 4*t^8.849 + 6*t^8.902 - t^4.3/y - (2*t^6.65)/y - (3*t^6.899)/y + (6*t^7.7)/y + (11*t^7.95)/y + (3*t^8.199)/y + (3*t^8.502)/y + (6*t^8.751)/y - t^4.3*y - 2*t^6.65*y - 3*t^6.899*y + 6*t^7.7*y + 11*t^7.95*y + 3*t^8.199*y + 3*t^8.502*y + 6*t^8.751*y 3*g1*t^2.35 + (3*t^2.599)/g1^4 + g1^9*t^3.151 + g1^4*t^3.401 + t^3.899/g1^6 + 2*g1^7*t^4.451 + 7*g1^2*t^4.7 + (8*t^4.95)/g1^3 + (5*t^5.199)/g1^8 + 4*g1^10*t^5.502 + 5*g1^5*t^5.751 - t^6. - t^6.249/g1^5 + g1^18*t^6.303 + (2*t^6.498)/g1^10 + g1^13*t^6.552 + 3*g1^8*t^6.801 + 13*g1^3*t^7.05 + (13*t^7.3)/g1^2 + (11*t^7.549)/g1^7 + 2*g1^16*t^7.602 + (9*t^7.798)/g1^12 + 9*g1^11*t^7.852 + 9*g1^6*t^8.101 - 4*g1*t^8.35 - (9*t^8.599)/g1^4 + 4*g1^19*t^8.653 - (4*t^8.849)/g1^9 + 6*g1^14*t^8.902 - t^4.3/(g1^2*y) - (2*t^6.65)/(g1*y) - (3*t^6.899)/(g1^6*y) + (6*g1^2*t^7.7)/y + (11*t^7.95)/(g1^3*y) + (3*t^8.199)/(g1^8*y) + (3*g1^10*t^8.502)/y + (6*g1^5*t^8.751)/y - (t^4.3*y)/g1^2 - (2*t^6.65*y)/g1 - (3*t^6.899*y)/g1^6 + 6*g1^2*t^7.7*y + (11*t^7.95*y)/g1^3 + (3*t^8.199*y)/g1^8 + 3*g1^10*t^8.502*y + 6*g1^5*t^8.751*y


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
47109 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ 0.6567 0.8222 0.7987 [M:[0.8639, 0.784, 1.216, 0.8639, 0.784], q:[0.7042, 0.4319], qb:[0.784, 0.3521], phi:[0.4319]] 2*t^2.352 + 3*t^2.592 + t^3.169 + t^3.408 + t^3.648 + t^3.887 + 2*t^4.465 + 4*t^4.704 + 5*t^4.944 + 5*t^5.183 + 3*t^5.521 + 4*t^5.76 + t^6. - t^4.296/y - t^4.296*y detail