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
58428 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ 1.4267 1.6897 0.8444 [X:[], M:[0.7922], q:[0.4103, 0.3948], qb:[0.3974, 0.3974], phi:[0.4]] [X:[], M:[[3]], q:[[-4], [2]], qb:[[1], [1]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ 2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ 3 3*t^2.38 + t^2.4 + 2*t^2.42 + 2*t^3.58 + t^3.6 + t^3.62 + 6*t^4.75 + 7*t^4.78 + 8*t^4.8 + 4*t^4.82 + 4*t^4.85 + 5*t^5.95 + 7*t^5.98 + 3*t^6. + 3*t^6.02 + 2*t^6.05 + 10*t^7.13 + 20*t^7.15 + 26*t^7.18 + 19*t^7.2 + 15*t^7.22 + 9*t^7.25 + 6*t^7.27 + t^7.29 + 9*t^8.33 + 19*t^8.35 + 8*t^8.38 + 11*t^8.4 + 2*t^8.42 + 6*t^8.45 + 2*t^8.47 - t^4.2/y - t^5.4/y - (3*t^6.58)/y - t^6.6/y - (2*t^6.62)/y + (3*t^7.75)/y + (5*t^7.8)/y + t^7.82/y + t^7.85/y - t^4.2*y - t^5.4*y - 3*t^6.58*y - t^6.6*y - 2*t^6.62*y + 3*t^7.75*y + 5*t^7.8*y + t^7.82*y + t^7.85*y 3*g1^3*t^2.38 + t^2.4 + (2*t^2.42)/g1^3 + 2*g1^3*t^3.58 + t^3.6 + t^3.62/g1^3 + 6*g1^6*t^4.75 + 7*g1^3*t^4.78 + 8*t^4.8 + (4*t^4.82)/g1^3 + (4*t^4.85)/g1^6 + 5*g1^6*t^5.95 + 7*g1^3*t^5.98 + 3*t^6. + (3*t^6.02)/g1^3 + (2*t^6.05)/g1^6 + 10*g1^9*t^7.13 + 20*g1^6*t^7.15 + 26*g1^3*t^7.18 + 19*t^7.2 + (15*t^7.22)/g1^3 + (9*t^7.25)/g1^6 + (6*t^7.27)/g1^9 + t^7.29/g1^12 + 9*g1^9*t^8.33 + 19*g1^6*t^8.35 + 8*g1^3*t^8.38 + 11*t^8.4 + (2*t^8.42)/g1^3 + (6*t^8.45)/g1^6 + (2*t^8.47)/g1^9 - t^4.2/y - t^5.4/y - (3*g1^3*t^6.58)/y - t^6.6/y - (2*t^6.62)/(g1^3*y) + (3*g1^6*t^7.75)/y + (5*t^7.8)/y + t^7.82/(g1^3*y) + t^7.85/(g1^6*y) - t^4.2*y - t^5.4*y - 3*g1^3*t^6.58*y - t^6.6*y - (2*t^6.62*y)/g1^3 + 3*g1^6*t^7.75*y + 5*t^7.8*y + (t^7.82*y)/g1^3 + (t^7.85*y)/g1^6


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
57350 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ 1.4268 1.6899 0.8443 [M:[0.7907], q:[0.4094, 0.3907], qb:[0.4, 0.4], phi:[0.4]] 3*t^2.372 + t^2.4 + 2*t^2.428 + 2*t^3.572 + t^3.6 + t^3.628 + 6*t^4.744 + 6*t^4.772 + 9*t^4.8 + 5*t^4.828 + 3*t^4.856 + 5*t^5.944 + 6*t^5.972 + 4*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail