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
46507 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ 0.6381 0.8353 0.764 [M:[0.9488, 0.8329, 0.8463, 0.8463], q:[0.7372, 0.314], qb:[0.4299, 0.4165], phi:[0.5256]] [M:[[-4], [26], [-12], [-12]], q:[[-1], [5]], qb:[[-25], [13]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ -1 t^2.191 + t^2.232 + t^2.499 + 3*t^2.539 + t^2.846 + t^3.154 + t^3.768 + t^3.809 + t^4.076 + t^4.116 + t^4.156 + t^4.383 + t^4.423 + t^4.463 + t^4.69 + 4*t^4.73 + 3*t^4.771 + t^4.998 + 4*t^5.038 + 7*t^5.078 + 2*t^5.345 + 4*t^5.385 + 2*t^5.693 - t^6. + 2*t^6.267 + 3*t^6.307 + 3*t^6.348 + t^6.388 + 2*t^6.574 + 4*t^6.615 + 4*t^6.655 + 4*t^6.695 + t^6.882 + 3*t^6.922 + 3*t^6.962 + 3*t^7.002 + t^7.189 + 4*t^7.229 + 7*t^7.27 + 7*t^7.31 + t^7.496 + 4*t^7.537 + 7*t^7.577 + 12*t^7.617 + 2*t^7.844 + 4*t^7.884 + 7*t^7.924 + t^7.965 + t^8.151 - 2*t^8.191 + 2*t^8.232 + t^8.272 + t^8.312 + t^8.459 - 3*t^8.499 - 6*t^8.539 + t^8.619 + 3*t^8.766 + 4*t^8.806 + t^8.846 + 6*t^8.887 + 4*t^8.927 - t^4.577/y - t^7.076/y - (2*t^7.116)/y + t^7.423/y + t^7.69/y + (4*t^7.73)/y + (3*t^7.771)/y + (6*t^8.038)/y + (5*t^8.078)/y + (2*t^8.345)/y + (4*t^8.385)/y + t^8.652/y + (3*t^8.693)/y + t^8.96/y - t^4.577*y - t^7.076*y - 2*t^7.116*y + t^7.423*y + t^7.69*y + 4*t^7.73*y + 3*t^7.771*y + 6*t^8.038*y + 5*t^8.078*y + 2*t^8.345*y + 4*t^8.385*y + t^8.652*y + 3*t^8.693*y + t^8.96*y g1^18*t^2.191 + t^2.232/g1^20 + g1^26*t^2.499 + (3*t^2.539)/g1^12 + t^2.846/g1^4 + g1^4*t^3.154 + g1^20*t^3.768 + t^3.809/g1^18 + g1^28*t^4.076 + t^4.116/g1^10 + t^4.156/g1^48 + g1^36*t^4.383 + t^4.423/g1^2 + t^4.463/g1^40 + g1^44*t^4.69 + 4*g1^6*t^4.73 + (3*t^4.771)/g1^32 + g1^52*t^4.998 + 4*g1^14*t^5.038 + (7*t^5.078)/g1^24 + 2*g1^22*t^5.345 + (4*t^5.385)/g1^16 + (2*t^5.693)/g1^8 - t^6. + 2*g1^46*t^6.267 + 3*g1^8*t^6.307 + (3*t^6.348)/g1^30 + t^6.388/g1^68 + 2*g1^54*t^6.574 + 4*g1^16*t^6.615 + (4*t^6.655)/g1^22 + (4*t^6.695)/g1^60 + g1^62*t^6.882 + 3*g1^24*t^6.922 + (3*t^6.962)/g1^14 + (3*t^7.002)/g1^52 + g1^70*t^7.189 + 4*g1^32*t^7.229 + (7*t^7.27)/g1^6 + (7*t^7.31)/g1^44 + g1^78*t^7.496 + 4*g1^40*t^7.537 + 7*g1^2*t^7.577 + (12*t^7.617)/g1^36 + 2*g1^48*t^7.844 + 4*g1^10*t^7.884 + (7*t^7.924)/g1^28 + t^7.965/g1^66 + g1^56*t^8.151 - 2*g1^18*t^8.191 + (2*t^8.232)/g1^20 + t^8.272/g1^58 + t^8.312/g1^96 + g1^64*t^8.459 - 3*g1^26*t^8.499 - (6*t^8.539)/g1^12 + t^8.619/g1^88 + 3*g1^72*t^8.766 + 4*g1^34*t^8.806 + t^8.846/g1^4 + (6*t^8.887)/g1^42 + (4*t^8.927)/g1^80 - (g1^2*t^4.577)/y - (g1^28*t^7.076)/y - (2*t^7.116)/(g1^10*y) + t^7.423/(g1^2*y) + (g1^44*t^7.69)/y + (4*g1^6*t^7.73)/y + (3*t^7.771)/(g1^32*y) + (6*g1^14*t^8.038)/y + (5*t^8.078)/(g1^24*y) + (2*g1^22*t^8.345)/y + (4*t^8.385)/(g1^16*y) + (g1^30*t^8.652)/y + (3*t^8.693)/(g1^8*y) + (g1^38*t^8.96)/y - g1^2*t^4.577*y - g1^28*t^7.076*y - (2*t^7.116*y)/g1^10 + (t^7.423*y)/g1^2 + g1^44*t^7.69*y + 4*g1^6*t^7.73*y + (3*t^7.771*y)/g1^32 + 6*g1^14*t^8.038*y + (5*t^8.078*y)/g1^24 + 2*g1^22*t^8.345*y + (4*t^8.385*y)/g1^16 + g1^30*t^8.652*y + (3*t^8.693*y)/g1^8 + g1^38*t^8.96*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
48258 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{5}$ 0.6334 0.8272 0.7657 [M:[0.9496, 0.8278, 0.8487, 0.8487, 1.0504], q:[0.7374, 0.313], qb:[0.4348, 0.4139], phi:[0.5252]] t^2.181 + t^2.243 + t^2.484 + 3*t^2.546 + 2*t^3.151 + t^3.757 + t^3.819 + t^4.059 + t^4.122 + t^4.184 + t^4.362 + t^4.424 + t^4.487 + t^4.664 + 4*t^4.727 + 3*t^4.79 + t^4.967 + 3*t^5.03 + 6*t^5.092 + 2*t^5.332 + 2*t^5.395 + t^5.635 + 4*t^5.697 - 2*t^6. - t^4.576/y - t^4.576*y detail
48115 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ 0.6576 0.8714 0.7546 [M:[0.9473, 0.8427, 0.8418, 0.8418, 0.7364], q:[0.7368, 0.3159], qb:[0.4205, 0.4213], phi:[0.5264]] 2*t^2.209 + t^2.212 + 3*t^2.526 + t^2.528 + t^2.842 + t^3.158 + t^3.788 + t^4.102 + t^4.105 + t^4.107 + 3*t^4.418 + 2*t^4.421 + t^4.423 + 6*t^4.735 + 5*t^4.737 + t^4.74 + 8*t^5.051 + 4*t^5.054 + t^5.056 + 5*t^5.367 + 2*t^5.37 + 2*t^5.684 + t^5.997 - 2*t^6. - t^4.579/y - t^4.579*y detail


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
46122 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ 0.625 0.8125 0.7692 [M:[0.9507, 0.8203, 0.8521], q:[0.7377, 0.3116], qb:[0.442, 0.4102], phi:[0.5246]] t^2.165 + t^2.261 + t^2.461 + 2*t^2.556 + t^2.852 + t^3.148 + t^3.444 + t^3.739 + t^3.835 + t^4.035 + t^4.13 + t^4.226 + t^4.331 + t^4.426 + t^4.521 + t^4.626 + 3*t^4.722 + 2*t^4.817 + t^4.922 + 3*t^5.017 + 4*t^5.113 + 2*t^5.313 + 3*t^5.409 + t^5.609 + 2*t^5.704 + t^5.905 + t^6. - t^4.574/y - t^4.574*y detail