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
1403 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{4}^{2}$ 0.7344 0.9115 0.8058 [M:[1.0, 0.8102, 0.8102, 1.0, 1.0, 0.8102], q:[0.5949, 0.4051], qb:[0.5949, 0.5949], phi:[0.4525]] [M:[[0], [-4], [-4], [0], [0], [-4]], q:[[2], [-2]], qb:[[2], [2]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$ ${}M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{5}$ -4 3*t^2.431 + t^2.715 + 3*t^3. + t^3.788 + 3*t^4.358 + 6*t^4.861 + 6*t^4.927 + 3*t^5.146 + 7*t^5.431 + 3*t^5.715 - 4*t^6. + 3*t^6.219 + t^6.504 - 4*t^6.569 + 9*t^6.788 + 2*t^7.073 + 10*t^7.292 + 15*t^7.358 + 7*t^7.576 + 3*t^7.642 + 12*t^7.861 + 6*t^7.927 + 10*t^8.146 - 6*t^8.212 - 12*t^8.431 - 3*t^8.496 + 6*t^8.649 + 2*t^8.715 + 3*t^8.934 - t^4.358/y - (3*t^6.788)/y - t^7.073/y + t^7.642/y + (3*t^7.861)/y + (3*t^7.927)/y + (3*t^8.146)/y + (9*t^8.431)/y + (3*t^8.715)/y - t^4.358*y - 3*t^6.788*y - t^7.073*y + t^7.642*y + 3*t^7.861*y + 3*t^7.927*y + 3*t^8.146*y + 9*t^8.431*y + 3*t^8.715*y (3*t^2.431)/g1^4 + t^2.715/g1^2 + 3*t^3. + t^3.788/g1^5 + (3*t^4.358)/g1 + (6*t^4.861)/g1^8 + 6*g1^3*t^4.927 + (3*t^5.146)/g1^6 + (7*t^5.431)/g1^4 + (3*t^5.715)/g1^2 - 4*t^6. + (3*t^6.219)/g1^9 + t^6.504/g1^7 - 4*g1^4*t^6.569 + (9*t^6.788)/g1^5 + (2*t^7.073)/g1^3 + (10*t^7.292)/g1^12 + (15*t^7.358)/g1 + (7*t^7.576)/g1^10 + 3*g1*t^7.642 + (12*t^7.861)/g1^8 + 6*g1^3*t^7.927 + (10*t^8.146)/g1^6 - 6*g1^5*t^8.212 - (12*t^8.431)/g1^4 - 3*g1^7*t^8.496 + (6*t^8.649)/g1^13 + (2*t^8.715)/g1^2 + (3*t^8.934)/g1^11 - t^4.358/(g1*y) - (3*t^6.788)/(g1^5*y) - t^7.073/(g1^3*y) + (g1*t^7.642)/y + (3*t^7.861)/(g1^8*y) + (3*g1^3*t^7.927)/y + (3*t^8.146)/(g1^6*y) + (9*t^8.431)/(g1^4*y) + (3*t^8.715)/(g1^2*y) - (t^4.358*y)/g1 - (3*t^6.788*y)/g1^5 - (t^7.073*y)/g1^3 + g1*t^7.642*y + (3*t^7.861*y)/g1^8 + 3*g1^3*t^7.927*y + (3*t^8.146*y)/g1^6 + (9*t^8.431*y)/g1^4 + (3*t^8.715*y)/g1^2


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
916 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ 0.7478 0.9314 0.8029 [M:[1.0, 0.7502, 0.889, 0.8612, 1.0, 0.7502], q:[0.5555, 0.4445], qb:[0.5555, 0.6943], phi:[0.4375]] 2*t^2.251 + t^2.584 + t^2.625 + t^2.667 + 2*t^3. + t^3.98 + 2*t^4.313 + 3*t^4.501 + 3*t^4.646 + t^4.729 + 2*t^4.834 + 2*t^4.876 + 2*t^4.917 + 2*t^5.062 + t^5.167 + t^5.209 + 5*t^5.251 + t^5.292 + t^5.334 + t^5.478 + 2*t^5.625 - 3*t^6. - t^4.313/y - t^4.313*y detail