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
3286 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{3}X_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ 0.6661 0.8451 0.7882 [X:[1.4579], M:[0.8812, 1.2203, 0.5421, 0.7797, 0.7797, 0.6782], q:[0.3391, 0.7797], qb:[0.4406, 0.6782], phi:[0.4406]] [X:[[7]], M:[[-4], [-1], [-7], [1], [1], [6]], q:[[3], [1]], qb:[[-2], [6]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{6}\phi_{1}q_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}q_{1}^{2}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }M_{6}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ ${}\phi_{1}^{3}q_{1}^{2}$, ${ }M_{4}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ 2 t^2.035 + 2*t^2.339 + 2*t^2.644 + t^3.052 + 2*t^3.356 + t^3.661 + t^4.069 + 4*t^4.374 + 6*t^4.678 + 3*t^4.983 + t^5.087 + 2*t^5.287 + 5*t^5.391 + 6*t^5.696 + 2*t^6. + 2*t^6.104 - 2*t^6.304 + 6*t^6.408 - t^6.609 + 10*t^6.713 + 8*t^7.017 + t^7.121 + 3*t^7.322 + 7*t^7.426 + t^7.626 + 13*t^7.73 + 3*t^7.931 + 9*t^8.035 + 2*t^8.138 - 4*t^8.339 + 9*t^8.443 - 7*t^8.644 + 17*t^8.747 - 5*t^8.948 - t^4.322/y - t^6.356/y - t^6.661/y - (2*t^6.965)/y + (2*t^7.374)/y + (5*t^7.678)/y + (5*t^7.983)/y + t^8.087/y + (2*t^8.287)/y + (3*t^8.391)/y + (6*t^8.696)/y - t^4.322*y - t^6.356*y - t^6.661*y - 2*t^6.965*y + 2*t^7.374*y + 5*t^7.678*y + 5*t^7.983*y + t^8.087*y + 2*t^8.287*y + 3*t^8.391*y + 6*t^8.696*y g1^6*t^2.035 + 2*g1*t^2.339 + (2*t^2.644)/g1^4 + g1^9*t^3.052 + 2*g1^4*t^3.356 + t^3.661/g1 + g1^12*t^4.069 + 4*g1^7*t^4.374 + 6*g1^2*t^4.678 + (3*t^4.983)/g1^3 + g1^15*t^5.087 + (2*t^5.287)/g1^8 + 5*g1^10*t^5.391 + 6*g1^5*t^5.696 + 2*t^6. + 2*g1^18*t^6.104 - (2*t^6.304)/g1^5 + 6*g1^13*t^6.408 - t^6.609/g1^10 + 10*g1^8*t^6.713 + 8*g1^3*t^7.017 + g1^21*t^7.121 + (3*t^7.322)/g1^2 + 7*g1^16*t^7.426 + t^7.626/g1^7 + 13*g1^11*t^7.73 + (3*t^7.931)/g1^12 + 9*g1^6*t^8.035 + 2*g1^24*t^8.138 - 4*g1*t^8.339 + 9*g1^19*t^8.443 - (7*t^8.644)/g1^4 + 17*g1^14*t^8.747 - (5*t^8.948)/g1^9 - t^4.322/(g1^2*y) - (g1^4*t^6.356)/y - t^6.661/(g1*y) - (2*t^6.965)/(g1^6*y) + (2*g1^7*t^7.374)/y + (5*g1^2*t^7.678)/y + (5*t^7.983)/(g1^3*y) + (g1^15*t^8.087)/y + (2*t^8.287)/(g1^8*y) + (3*g1^10*t^8.391)/y + (6*g1^5*t^8.696)/y - (t^4.322*y)/g1^2 - g1^4*t^6.356*y - (t^6.661*y)/g1 - (2*t^6.965*y)/g1^6 + 2*g1^7*t^7.374*y + 5*g1^2*t^7.678*y + (5*t^7.983*y)/g1^3 + g1^15*t^8.087*y + (2*t^8.287*y)/g1^8 + 3*g1^10*t^8.391*y + 6*g1^5*t^8.696*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
2772 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{3}X_{1}$ + ${ }M_{2}M_{5}$ 0.6453 0.804 0.8026 [X:[1.4612], M:[0.8793, 1.2198, 0.5388, 0.7802, 0.7802], q:[0.3405, 0.7802], qb:[0.4397, 0.681], phi:[0.4397]] 2*t^2.34 + 2*t^2.638 + t^3.064 + 2*t^3.362 + t^3.66 + t^3.957 + 2*t^4.383 + 4*t^4.681 + 3*t^4.979 + 2*t^5.276 + 3*t^5.405 + 5*t^5.702 + 2*t^6. - t^4.319/y - t^4.319*y detail