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
53332 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}q_{1}^{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ 0.6664 0.8401 0.7931 [M:[1.171, 0.7323, 0.829, 0.829, 0.829, 0.7806], q:[0.4145, 0.4145], qb:[0.8532, 0.7565], phi:[0.3903]] [M:[[6], [14], [-6], [-6], [-6], [4]], q:[[-3], [-3]], qb:[[-11], [9]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$ ${}M_{6}\phi_{1}q_{1}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$ 0 t^2.197 + 2*t^2.342 + 3*t^2.487 + 2*t^3.658 + t^3.803 + t^4.394 + 2*t^4.539 + 6*t^4.684 + 7*t^4.829 + 6*t^4.974 + 6*t^6.145 + 3*t^6.29 + t^6.59 + 2*t^6.736 + 6*t^6.881 + 9*t^7.026 + 11*t^7.171 + 11*t^7.316 + 10*t^7.461 + t^7.606 - 4*t^8.197 - 5*t^8.342 - 3*t^8.487 + 11*t^8.632 + 6*t^8.777 + t^8.787 + 2*t^8.932 - t^4.171/y - t^6.368/y - (2*t^6.513)/y - (2*t^6.658)/y + (2*t^7.539)/y + (6*t^7.684)/y + (8*t^7.829)/y + (4*t^7.974)/y - t^8.565/y - (2*t^8.71)/y - (3*t^8.855)/y - t^4.171*y - t^6.368*y - 2*t^6.513*y - 2*t^6.658*y + 2*t^7.539*y + 6*t^7.684*y + 8*t^7.829*y + 4*t^7.974*y - t^8.565*y - 2*t^8.71*y - 3*t^8.855*y g1^14*t^2.197 + 2*g1^4*t^2.342 + (3*t^2.487)/g1^6 + (2*t^3.658)/g1^4 + t^3.803/g1^14 + g1^28*t^4.394 + 2*g1^18*t^4.539 + 6*g1^8*t^4.684 + (7*t^4.829)/g1^2 + (6*t^4.974)/g1^12 + (6*t^6.145)/g1^10 + (3*t^6.29)/g1^20 + g1^42*t^6.59 + 2*g1^32*t^6.736 + 6*g1^22*t^6.881 + 9*g1^12*t^7.026 + 11*g1^2*t^7.171 + (11*t^7.316)/g1^8 + (10*t^7.461)/g1^18 + t^7.606/g1^28 - 4*g1^14*t^8.197 - 5*g1^4*t^8.342 - (3*t^8.487)/g1^6 + (11*t^8.632)/g1^16 + (6*t^8.777)/g1^26 + g1^56*t^8.787 + 2*g1^46*t^8.932 - (g1^2*t^4.171)/y - (g1^16*t^6.368)/y - (2*g1^6*t^6.513)/y - (2*t^6.658)/(g1^4*y) + (2*g1^18*t^7.539)/y + (6*g1^8*t^7.684)/y + (8*t^7.829)/(g1^2*y) + (4*t^7.974)/(g1^12*y) - (g1^30*t^8.565)/y - (2*g1^20*t^8.71)/y - (3*g1^10*t^8.855)/y - g1^2*t^4.171*y - g1^16*t^6.368*y - 2*g1^6*t^6.513*y - (2*t^6.658*y)/g1^4 + 2*g1^18*t^7.539*y + 6*g1^8*t^7.684*y + (8*t^7.829*y)/g1^2 + (4*t^7.974*y)/g1^12 - g1^30*t^8.565*y - 2*g1^20*t^8.71*y - 3*g1^10*t^8.855*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
48303 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}q_{1}^{2}$ + ${ }M_{1}M_{5}$ 0.6488 0.8093 0.8017 [M:[1.1755, 0.7428, 0.8245, 0.8245, 0.8245], q:[0.4123, 0.4123], qb:[0.845, 0.7632], phi:[0.3918]] t^2.228 + t^2.351 + 3*t^2.474 + 3*t^3.649 + t^3.772 + t^4.457 + t^4.579 + 4*t^4.702 + 4*t^4.825 + 6*t^4.947 + t^5.877 - t^6. - t^4.175/y - t^4.175*y detail