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
46366 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ 0.5861 0.7654 0.7658 [M:[1.0, 0.7055, 0.8528, 0.7055], q:[0.7868, 0.2132], qb:[0.5077, 0.7868], phi:[0.4264]] [M:[[0], [-8], [-4], [-8]], q:[[1], [-1]], qb:[[7], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}^{4}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$ ${}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ -1 2*t^2.117 + t^2.163 + 3*t^2.558 + 2*t^3. + 3*t^4.233 + 2*t^4.279 + 2*t^4.325 + 6*t^4.675 + 4*t^4.721 + 9*t^5.117 + 2*t^5.163 + 4*t^5.558 - t^6. + 4*t^6.35 + 2*t^6.396 + 2*t^6.488 + 9*t^6.791 + 6*t^6.837 + 3*t^6.883 + 16*t^7.233 + 9*t^7.279 + 2*t^7.325 + 15*t^7.675 + 2*t^7.721 - t^7.767 + 2*t^8.117 - 4*t^8.163 + 5*t^8.466 + 2*t^8.512 - 7*t^8.558 - 2*t^8.604 + 3*t^8.65 + 12*t^8.908 + 6*t^8.954 - t^4.279/y - (2*t^6.396)/y - (2*t^6.837)/y + t^7.233/y + (2*t^7.279)/y + (6*t^7.675)/y + (5*t^7.721)/y + (7*t^8.117)/y + (4*t^8.163)/y - (3*t^8.512)/y + (6*t^8.558)/y - (4*t^8.954)/y - t^4.279*y - 2*t^6.396*y - 2*t^6.837*y + t^7.233*y + 2*t^7.279*y + 6*t^7.675*y + 5*t^7.721*y + 7*t^8.117*y + 4*t^8.163*y - 3*t^8.512*y + 6*t^8.558*y - 4*t^8.954*y (2*t^2.117)/g1^8 + g1^6*t^2.163 + (3*t^2.558)/g1^4 + 2*t^3. + (3*t^4.233)/g1^16 + (2*t^4.279)/g1^2 + 2*g1^12*t^4.325 + (6*t^4.675)/g1^12 + 4*g1^2*t^4.721 + (9*t^5.117)/g1^8 + 2*g1^6*t^5.163 + (4*t^5.558)/g1^4 - t^6. + (4*t^6.35)/g1^24 + (2*t^6.396)/g1^10 + 2*g1^18*t^6.488 + (9*t^6.791)/g1^20 + (6*t^6.837)/g1^6 + 3*g1^8*t^6.883 + (16*t^7.233)/g1^16 + (9*t^7.279)/g1^2 + 2*g1^12*t^7.325 + (15*t^7.675)/g1^12 + 2*g1^2*t^7.721 - g1^16*t^7.767 + (2*t^8.117)/g1^8 - 4*g1^6*t^8.163 + (5*t^8.466)/g1^32 + (2*t^8.512)/g1^18 - (7*t^8.558)/g1^4 - 2*g1^10*t^8.604 + 3*g1^24*t^8.65 + (12*t^8.908)/g1^28 + (6*t^8.954)/g1^14 - t^4.279/(g1^2*y) - (2*t^6.396)/(g1^10*y) - (2*t^6.837)/(g1^6*y) + t^7.233/(g1^16*y) + (2*t^7.279)/(g1^2*y) + (6*t^7.675)/(g1^12*y) + (5*g1^2*t^7.721)/y + (7*t^8.117)/(g1^8*y) + (4*g1^6*t^8.163)/y - (3*t^8.512)/(g1^18*y) + (6*t^8.558)/(g1^4*y) - (4*t^8.954)/(g1^14*y) - (t^4.279*y)/g1^2 - (2*t^6.396*y)/g1^10 - (2*t^6.837*y)/g1^6 + (t^7.233*y)/g1^16 + (2*t^7.279*y)/g1^2 + (6*t^7.675*y)/g1^12 + 5*g1^2*t^7.721*y + (7*t^8.117*y)/g1^8 + 4*g1^6*t^8.163*y - (3*t^8.512*y)/g1^18 + (6*t^8.558*y)/g1^4 - (4*t^8.954*y)/g1^14


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
46184 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ 0.5658 0.7265 0.7788 [M:[1.0, 0.7154, 0.8577], q:[0.7856, 0.2144], qb:[0.499, 0.7856], phi:[0.4289]] t^2.14 + t^2.146 + 3*t^2.573 + 2*t^3. + t^3.854 + 2*t^4.281 + t^4.287 + t^4.293 + 4*t^4.713 + 3*t^4.719 + 2*t^5.14 + 7*t^5.146 + 4*t^5.573 + t^5.994 - t^4.287/y - t^4.287*y detail