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
60984 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ 1.1496 1.3617 0.8442 [X:[1.3684], M:[0.9737, 0.6842], q:[0.7281, 0.0965], qb:[0.5877, 0.5351], phi:[0.3421]] [X:[[12]], M:[[-9], [6]], q:[[-17], [-5]], qb:[[11], [-7]], phi:[[3]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}^{2}$, ${ }M_{2}\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}q_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$ ${}M_{2}\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}^{5}q_{2}^{3}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}^{4}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ 2}\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ 5 3*t^2.05 + 2*t^2.92 + t^3.08 + 2*t^3.79 + 2*t^3.95 + 7*t^4.11 + 2*t^4.82 + 7*t^4.97 + 2*t^5.13 + t^5.68 + 9*t^5.84 + 5*t^6. + 13*t^6.16 + 4*t^6.71 + 7*t^6.87 + 15*t^7.03 + 3*t^7.18 + 3*t^7.58 + 8*t^7.74 + 22*t^7.89 + 7*t^8.05 + 20*t^8.21 + 5*t^8.61 + 17*t^8.76 + 8*t^8.92 - t^4.03/y - t^5.05/y - (3*t^6.08)/y - t^6.95/y - t^7.82/y + (5*t^7.97)/y - (4*t^8.13)/y + (6*t^8.84)/y - t^4.03*y - t^5.05*y - 3*t^6.08*y - t^6.95*y - t^7.82*y + 5*t^7.97*y - 4*t^8.13*y + 6*t^8.84*y 3*g1^6*t^2.05 + (2*t^2.92)/g1^9 + g1^9*t^3.08 + (2*t^3.79)/g1^24 + (2*t^3.95)/g1^6 + 7*g1^12*t^4.11 + (2*t^4.82)/g1^21 + (7*t^4.97)/g1^3 + 2*g1^15*t^5.13 + t^5.68/g1^36 + (9*t^5.84)/g1^18 + 5*t^6. + 13*g1^18*t^6.16 + (4*t^6.71)/g1^33 + (7*t^6.87)/g1^15 + 15*g1^3*t^7.03 + 3*g1^21*t^7.18 + (3*t^7.58)/g1^48 + (8*t^7.74)/g1^30 + (22*t^7.89)/g1^12 + 7*g1^6*t^8.05 + 20*g1^24*t^8.21 + (5*t^8.61)/g1^45 + (17*t^8.76)/g1^27 + (8*t^8.92)/g1^9 - (g1^3*t^4.03)/y - (g1^6*t^5.05)/y - (3*g1^9*t^6.08)/y - t^6.95/(g1^6*y) - t^7.82/(g1^21*y) + (5*t^7.97)/(g1^3*y) - (4*g1^15*t^8.13)/y + (6*t^8.84)/(g1^18*y) - g1^3*t^4.03*y - g1^6*t^5.05*y - 3*g1^9*t^6.08*y - (t^6.95*y)/g1^6 - (t^7.82*y)/g1^21 + (5*t^7.97*y)/g1^3 - 4*g1^15*t^8.13*y + (6*t^8.84*y)/g1^18


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
58875 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ 1.2527 1.4758 0.8488 [X:[1.4684], M:[0.8987, 0.7342], q:[0.7425, 0.211], qb:[0.5232, 0.3206], phi:[0.3671]] 3*t^2.2 + 2*t^2.7 + t^3.19 + t^3.3 + t^3.8 + t^4.29 + 7*t^4.41 + 2*t^4.59 + 7*t^4.9 + 2*t^5.2 + 6*t^5.39 + 2*t^5.51 + 2*t^5.7 + 2*t^5.89 + 2*t^6. - t^4.1/y - t^5.2/y - t^4.1*y - t^5.2*y detail