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
4222 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{1}q_{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{2}M_{8}$ 0.6713 0.8402 0.7989 [M:[1.1594, 1.087, 0.9493, 0.8406, 0.7029, 0.8768, 1.0507, 0.913], q:[0.7717, 0.3515], qb:[0.4891, 0.5616], phi:[0.4565]] [M:[[8], [-4], [10], [-8], [6], [-2], [-10], [4]], q:[[-1], [3]], qb:[[-11], [1]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }M_{4}$, ${ }M_{6}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{4}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{1}$ ${}$ -2 t^2.109 + t^2.522 + t^2.63 + 2*t^2.739 + t^3.152 + t^3.478 + t^3.783 + t^4. + t^4.109 + t^4.217 + t^4.304 + t^4.522 + t^4.63 + 2*t^4.739 + 2*t^4.848 + t^5.043 + t^5.152 + 4*t^5.261 + t^5.37 + 3*t^5.478 + t^5.674 + 3*t^5.891 - 2*t^6. + t^6.109 + 2*t^6.217 + 2*t^6.304 + t^6.326 + t^6.413 + t^6.522 + t^6.63 + t^6.739 + t^6.826 + 3*t^6.848 + 2*t^6.935 + 2*t^6.957 + 2*t^7.043 + t^7.152 + 3*t^7.261 + 2*t^7.37 + t^7.456 + 3*t^7.478 + t^7.565 + 3*t^7.587 + t^7.674 + 3*t^7.783 + 2*t^7.891 + 5*t^8. + t^8.087 - 2*t^8.109 + t^8.196 + 5*t^8.217 + t^8.304 + 3*t^8.413 + t^8.435 - t^8.522 + t^8.609 + t^8.63 - 4*t^8.739 + 3*t^8.826 + t^8.848 + t^8.935 + 4*t^8.957 - t^4.37/y - t^6.478/y - t^7./y - t^7.109/y + (2*t^7.63)/y + (2*t^7.739)/y + (2*t^7.848)/y + t^8.152/y + (4*t^8.261)/y + (2*t^8.37)/y + t^8.478/y + t^8.674/y + t^8.783/y + (3*t^8.891)/y - t^4.37*y - t^6.478*y - t^7.*y - t^7.109*y + 2*t^7.63*y + 2*t^7.739*y + 2*t^7.848*y + t^8.152*y + 4*t^8.261*y + 2*t^8.37*y + t^8.478*y + t^8.674*y + t^8.783*y + 3*t^8.891*y g1^6*t^2.109 + t^2.522/g1^8 + t^2.63/g1^2 + 2*g1^4*t^2.739 + t^3.152/g1^10 + g1^8*t^3.478 + t^3.783/g1^12 + t^4. + g1^6*t^4.109 + g1^12*t^4.217 + t^4.304/g1^20 + t^4.522/g1^8 + t^4.63/g1^2 + 2*g1^4*t^4.739 + 2*g1^10*t^4.848 + t^5.043/g1^16 + t^5.152/g1^10 + (4*t^5.261)/g1^4 + g1^2*t^5.37 + 3*g1^8*t^5.478 + t^5.674/g1^18 + (3*t^5.891)/g1^6 - 2*t^6. + g1^6*t^6.109 + 2*g1^12*t^6.217 + (2*t^6.304)/g1^20 + g1^18*t^6.326 + t^6.413/g1^14 + t^6.522/g1^8 + t^6.63/g1^2 + g1^4*t^6.739 + t^6.826/g1^28 + 3*g1^10*t^6.848 + (2*t^6.935)/g1^22 + 2*g1^16*t^6.957 + (2*t^7.043)/g1^16 + t^7.152/g1^10 + (3*t^7.261)/g1^4 + 2*g1^2*t^7.37 + t^7.456/g1^30 + 3*g1^8*t^7.478 + t^7.565/g1^24 + 3*g1^14*t^7.587 + t^7.674/g1^18 + (3*t^7.783)/g1^12 + (2*t^7.891)/g1^6 + 5*t^8. + t^8.087/g1^32 - 2*g1^6*t^8.109 + t^8.196/g1^26 + 5*g1^12*t^8.217 + t^8.304/g1^20 + (3*t^8.413)/g1^14 + g1^24*t^8.435 - t^8.522/g1^8 + t^8.609/g1^40 + t^8.63/g1^2 - 4*g1^4*t^8.739 + (3*t^8.826)/g1^28 + g1^10*t^8.848 + t^8.935/g1^22 + 4*g1^16*t^8.957 - (g1^2*t^4.37)/y - (g1^8*t^6.478)/y - t^7./y - (g1^6*t^7.109)/y + (2*t^7.63)/(g1^2*y) + (2*g1^4*t^7.739)/y + (2*g1^10*t^7.848)/y + t^8.152/(g1^10*y) + (4*t^8.261)/(g1^4*y) + (2*g1^2*t^8.37)/y + (g1^8*t^8.478)/y + t^8.674/(g1^18*y) + t^8.783/(g1^12*y) + (3*t^8.891)/(g1^6*y) - g1^2*t^4.37*y - g1^8*t^6.478*y - t^7.*y - g1^6*t^7.109*y + (2*t^7.63*y)/g1^2 + 2*g1^4*t^7.739*y + 2*g1^10*t^7.848*y + (t^8.152*y)/g1^10 + (4*t^8.261*y)/g1^4 + 2*g1^2*t^8.37*y + g1^8*t^8.478*y + (t^8.674*y)/g1^18 + (t^8.783*y)/g1^12 + (3*t^8.891*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
2218 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{1}q_{2}$ + ${ }M_{3}M_{7}$ 0.6635 0.8279 0.8015 [M:[1.1701, 1.0816, 0.9627, 0.8299, 0.7109, 0.8741, 1.0373], q:[0.7704, 0.3555], qb:[0.4744, 0.5629], phi:[0.4592]] t^2.133 + t^2.49 + t^2.622 + t^2.755 + t^3.112 + t^3.245 + t^3.51 + t^3.734 + t^4. + t^4.133 + t^4.224 + t^4.266 + t^4.49 + t^4.622 + 2*t^4.755 + t^4.888 + t^4.979 + t^5.112 + 3*t^5.245 + t^5.378 + t^5.51 + t^5.602 + t^5.734 + 3*t^5.867 - t^6. - t^4.378/y - t^4.378*y detail