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
2763 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}q_{2}$ 0.688 0.8991 0.7652 [M:[1.1225, 0.6887, 0.6887, 0.8113, 0.8113], q:[0.75, 0.4387], qb:[0.4387, 0.3725], phi:[0.5]] [M:[[2], [-1], [-1], [1], [1]], q:[[0], [-1]], qb:[[-1], [2]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{3}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}$ -5 2*t^2.066 + 4*t^2.434 + t^3. + 2*t^3.368 + t^3.735 + 6*t^4.132 + 8*t^4.5 + 10*t^4.868 + 2*t^5.066 + 8*t^5.434 + 8*t^5.801 - 5*t^6. + 4*t^6.169 + 8*t^6.199 + 20*t^6.566 + 3*t^6.735 + 16*t^6.934 + 2*t^7.103 + 2*t^7.132 + 16*t^7.301 + t^7.47 + 12*t^7.5 - 4*t^7.699 + 24*t^7.868 - 14*t^8.066 + 20*t^8.235 + 15*t^8.265 - 20*t^8.434 + 10*t^8.603 + 24*t^8.632 + 4*t^8.801 - t^4.5/y - (2*t^6.566)/y - (2*t^6.934)/y + (2*t^7.132)/y + (8*t^7.5)/y + (5*t^7.868)/y + (4*t^8.066)/y + (10*t^8.434)/y - (3*t^8.632)/y + (10*t^8.801)/y - t^4.5*y - 2*t^6.566*y - 2*t^6.934*y + 2*t^7.132*y + 8*t^7.5*y + 5*t^7.868*y + 4*t^8.066*y + 10*t^8.434*y - 3*t^8.632*y + 10*t^8.801*y (2*t^2.066)/g1 + 4*g1*t^2.434 + t^3. + 2*g1^2*t^3.368 + g1^4*t^3.735 + (6*t^4.132)/g1^2 + 8*t^4.5 + 10*g1^2*t^4.868 + (2*t^5.066)/g1 + 8*g1*t^5.434 + 8*g1^3*t^5.801 - 5*t^6. + 4*g1^5*t^6.169 + (8*t^6.199)/g1^3 + (20*t^6.566)/g1 + 3*g1^4*t^6.735 + 16*g1*t^6.934 + 2*g1^6*t^7.103 + (2*t^7.132)/g1^2 + 16*g1^3*t^7.301 + g1^8*t^7.47 + 12*t^7.5 - (4*t^7.699)/g1^3 + 24*g1^2*t^7.868 - (14*t^8.066)/g1 + 20*g1^4*t^8.235 + (15*t^8.265)/g1^4 - 20*g1*t^8.434 + 10*g1^6*t^8.603 + (24*t^8.632)/g1^2 + 4*g1^3*t^8.801 - t^4.5/y - (2*t^6.566)/(g1*y) - (2*g1*t^6.934)/y + (2*t^7.132)/(g1^2*y) + (8*t^7.5)/y + (5*g1^2*t^7.868)/y + (4*t^8.066)/(g1*y) + (10*g1*t^8.434)/y - (3*t^8.632)/(g1^2*y) + (10*g1^3*t^8.801)/y - t^4.5*y - (2*t^6.566*y)/g1 - 2*g1*t^6.934*y + (2*t^7.132*y)/g1^2 + 8*t^7.5*y + 5*g1^2*t^7.868*y + (4*t^8.066*y)/g1 + 10*g1*t^8.434*y - (3*t^8.632*y)/g1^2 + 10*g1^3*t^8.801*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
1758 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ 0.6724 0.8714 0.7716 [M:[1.1326, 0.6837, 0.6837, 0.8163], q:[0.75, 0.4337], qb:[0.4337, 0.3826], phi:[0.5]] 2*t^2.051 + 3*t^2.449 + t^3. + 2*t^3.398 + t^3.551 + t^3.795 + 6*t^4.102 + 6*t^4.5 + 6*t^4.898 + 2*t^5.051 + 7*t^5.449 + 2*t^5.602 + 6*t^5.846 - 2*t^6. - t^4.5/y - t^4.5*y detail