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
2064 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}^{4}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ 0.6577 0.8352 0.7876 [M:[0.8227, 1.1773, 0.8227, 0.6773, 1.3227, 0.8387], q:[0.75, 0.4273], qb:[0.4113, 0.4113], phi:[0.5]] [M:[[2], [-2], [2], [-2], [2], [-1]], q:[[0], [-2]], qb:[[1], [1]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }M_{3}$, ${ }M_{6}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$ ${}M_{6}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ -2 2*t^2.468 + 3*t^2.516 + t^3. + t^3.484 + 3*t^3.968 + 2*t^4.016 + t^4.064 + 3*t^4.936 + 6*t^4.984 + 6*t^5.032 + 2*t^5.468 + 3*t^5.516 - 2*t^6. - 2*t^6.048 + 6*t^6.436 + 10*t^6.484 + 6*t^6.532 + 3*t^6.58 - 2*t^7.016 + 4*t^7.404 + 8*t^7.452 + 6*t^7.5 + 7*t^7.548 + 8*t^7.936 + 8*t^7.984 + 8*t^8.032 + 2*t^8.08 + t^8.128 - t^8.42 - 10*t^8.468 - 13*t^8.516 - 6*t^8.564 + 9*t^8.904 + 16*t^8.952 - t^4.5/y - t^6.968/y - t^7.016/y + t^7.936/y + (7*t^7.984)/y + (4*t^8.032)/y + (2*t^8.468)/y + (3*t^8.516)/y + (2*t^8.952)/y - t^4.5*y - t^6.968*y - t^7.016*y + t^7.936*y + 7*t^7.984*y + 4*t^8.032*y + 2*t^8.468*y + 3*t^8.516*y + 2*t^8.952*y 2*g1^2*t^2.468 + (3*t^2.516)/g1 + t^3. + g1*t^3.484 + 3*g1^2*t^3.968 + (2*t^4.016)/g1 + t^4.064/g1^4 + 3*g1^4*t^4.936 + 6*g1*t^4.984 + (6*t^5.032)/g1^2 + 2*g1^2*t^5.468 + (3*t^5.516)/g1 - 2*t^6. - (2*t^6.048)/g1^3 + 6*g1^4*t^6.436 + 10*g1*t^6.484 + (6*t^6.532)/g1^2 + (3*t^6.58)/g1^5 - (2*t^7.016)/g1 + 4*g1^6*t^7.404 + 8*g1^3*t^7.452 + 6*t^7.5 + (7*t^7.548)/g1^3 + 8*g1^4*t^7.936 + 8*g1*t^7.984 + (8*t^8.032)/g1^2 + (2*t^8.08)/g1^5 + t^8.128/g1^8 - g1^5*t^8.42 - 10*g1^2*t^8.468 - (13*t^8.516)/g1 - (6*t^8.564)/g1^4 + 9*g1^6*t^8.904 + 16*g1^3*t^8.952 - t^4.5/y - (g1^2*t^6.968)/y - t^7.016/(g1*y) + (g1^4*t^7.936)/y + (7*g1*t^7.984)/y + (4*t^8.032)/(g1^2*y) + (2*g1^2*t^8.468)/y + (3*t^8.516)/(g1*y) + (2*g1^3*t^8.952)/y - t^4.5*y - g1^2*t^6.968*y - (t^7.016*y)/g1 + g1^4*t^7.936*y + 7*g1*t^7.984*y + (4*t^8.032*y)/g1^2 + 2*g1^2*t^8.468*y + (3*t^8.516*y)/g1 + 2*g1^3*t^8.952*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


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
878 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}^{4}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}M_{5}$ 0.644 0.812 0.7931 [M:[0.8115, 1.1885, 0.8115, 0.6885, 1.3115], q:[0.75, 0.4385], qb:[0.4058, 0.4058], phi:[0.5]] 2*t^2.435 + 2*t^2.533 + t^3. + 2*t^3.467 + 3*t^3.935 + 2*t^4.033 + t^4.131 + 3*t^4.869 + 4*t^4.967 + 3*t^5.065 + 2*t^5.435 + 2*t^5.533 + 2*t^5.902 - t^6. - t^4.5/y - t^4.5*y detail