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
4102 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}q_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{8}$ 0.6691 0.8502 0.787 [M:[1.1775, 1.215, 0.7475, 0.8225, 0.8225, 0.7475, 0.71, 0.8225], q:[0.8037, 0.4487], qb:[0.3738, 0.8037], phi:[0.3925]] [M:[[-6], [4], [-14], [6], [6], [-14], [-24], [6]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{7}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{8}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{7}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{8}$, ${ }M_{6}M_{8}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{8}$, ${ }M_{5}M_{8}$, ${ }M_{8}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{7}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{6}$, ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$ ${}\phi_{1}\tilde{q}_{2}^{2}$ -3 t^2.13 + 2*t^2.243 + 3*t^2.467 + t^3.42 + 2*t^3.645 + t^4.26 + 2*t^4.373 + 3*t^4.485 + 3*t^4.598 + 6*t^4.71 + t^4.822 + 6*t^4.935 + t^5.55 + 2*t^5.663 + t^5.775 + 5*t^5.888 - 3*t^6. + 4*t^6.112 - t^6.225 + t^6.39 + 2*t^6.503 + 3*t^6.615 + 7*t^6.728 + 7*t^6.84 + 9*t^6.953 + 7*t^7.065 + 8*t^7.178 + t^7.29 + 7*t^7.402 - t^7.515 + t^7.68 + 2*t^7.793 + 4*t^7.905 + 3*t^8.018 + 5*t^8.13 - 5*t^8.243 + 6*t^8.355 - 11*t^8.467 + t^8.521 + 4*t^8.58 + 2*t^8.633 - 4*t^8.692 + 3*t^8.745 + 7*t^8.858 + 12*t^8.97 - t^4.178/y - t^6.308/y - (2*t^6.42)/y - (2*t^6.645)/y + (2*t^7.373)/y + t^7.485/y + (3*t^7.598)/y + (8*t^7.71)/y + (5*t^7.935)/y + t^8.047/y - t^8.438/y - t^8.55/y - t^8.663/y + (3*t^8.888)/y - t^4.178*y - t^6.308*y - 2*t^6.42*y - 2*t^6.645*y + 2*t^7.373*y + t^7.485*y + 3*t^7.598*y + 8*t^7.71*y + 5*t^7.935*y + t^8.047*y - t^8.438*y - t^8.55*y - t^8.663*y + 3*t^8.888*y t^2.13/g1^24 + (2*t^2.243)/g1^14 + 3*g1^6*t^2.467 + t^3.42/g1^16 + 2*g1^4*t^3.645 + t^4.26/g1^48 + (2*t^4.373)/g1^38 + (3*t^4.485)/g1^28 + (3*t^4.598)/g1^18 + (6*t^4.71)/g1^8 + g1^2*t^4.822 + 6*g1^12*t^4.935 + t^5.55/g1^40 + (2*t^5.663)/g1^30 + t^5.775/g1^20 + (5*t^5.888)/g1^10 - 3*t^6. + 4*g1^10*t^6.112 - g1^20*t^6.225 + t^6.39/g1^72 + (2*t^6.503)/g1^62 + (3*t^6.615)/g1^52 + (7*t^6.728)/g1^42 + (7*t^6.84)/g1^32 + (9*t^6.953)/g1^22 + (7*t^7.065)/g1^12 + (8*t^7.178)/g1^2 + g1^8*t^7.29 + 7*g1^18*t^7.402 - g1^28*t^7.515 + t^7.68/g1^64 + (2*t^7.793)/g1^54 + (4*t^7.905)/g1^44 + (3*t^8.018)/g1^34 + (5*t^8.13)/g1^24 - (5*t^8.243)/g1^14 + (6*t^8.355)/g1^4 - 11*g1^6*t^8.467 + t^8.521/g1^96 + 4*g1^16*t^8.58 + (2*t^8.633)/g1^86 - 4*g1^26*t^8.692 + (3*t^8.745)/g1^76 + (7*t^8.858)/g1^66 + (12*t^8.97)/g1^56 - t^4.178/(g1^2*y) - t^6.308/(g1^26*y) - (2*t^6.42)/(g1^16*y) - (2*g1^4*t^6.645)/y + (2*t^7.373)/(g1^38*y) + t^7.485/(g1^28*y) + (3*t^7.598)/(g1^18*y) + (8*t^7.71)/(g1^8*y) + (5*g1^12*t^7.935)/y + (g1^22*t^8.047)/y - t^8.438/(g1^50*y) - t^8.55/(g1^40*y) - t^8.663/(g1^30*y) + (3*t^8.888)/(g1^10*y) - (t^4.178*y)/g1^2 - (t^6.308*y)/g1^26 - (2*t^6.42*y)/g1^16 - 2*g1^4*t^6.645*y + (2*t^7.373*y)/g1^38 + (t^7.485*y)/g1^28 + (3*t^7.598*y)/g1^18 + (8*t^7.71*y)/g1^8 + 5*g1^12*t^7.935*y + g1^22*t^8.047*y - (t^8.438*y)/g1^50 - (t^8.55*y)/g1^40 - (t^8.663*y)/g1^30 + (3*t^8.888*y)/g1^10


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
2118 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}q_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ 0.6541 0.825 0.7928 [M:[1.1748, 1.2168, 0.7412, 0.8252, 0.8252, 0.7412, 0.6992], q:[0.8042, 0.4546], qb:[0.3706, 0.8042], phi:[0.3916]] t^2.098 + 2*t^2.224 + 2*t^2.476 + t^3.398 + t^3.524 + 2*t^3.65 + t^4.195 + 2*t^4.321 + 3*t^4.447 + 2*t^4.573 + 4*t^4.699 + t^4.825 + 3*t^4.951 + t^5.496 + 3*t^5.622 + 3*t^5.748 + 4*t^5.874 - t^6. - t^4.175/y - t^4.175*y detail