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
297 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ 0.566 0.7275 0.778 [M:[0.9861, 1.0139, 0.8593, 0.7047], q:[0.5811, 0.9892], qb:[0.4328, 0.2782], phi:[0.4297]] [M:[[-1, 5], [1, -5], [-2, -2], [-5, 1]], q:[[-2, -5], [3, 6]], qb:[[3, 0], [0, 3]], phi:[[-1, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}$ -3 t^2.114 + t^2.133 + 3*t^2.578 + t^2.958 + t^3.042 + t^3.802 + t^4.228 + t^4.247 + 2*t^4.266 + 3*t^4.692 + 4*t^4.711 + t^5.072 + t^5.091 + 6*t^5.156 + t^5.175 + 2*t^5.536 + 2*t^5.62 + 2*t^5.916 + t^5.935 - 3*t^6. + t^6.084 + t^6.343 + t^6.361 + 3*t^6.38 + 2*t^6.399 - t^6.445 - 2*t^6.464 + t^6.761 + 3*t^6.806 + 3*t^6.825 + 4*t^6.844 - t^6.909 + t^7.187 + t^7.205 + t^7.224 + 6*t^7.27 + 6*t^7.289 + t^7.308 + t^7.605 + 2*t^7.65 + t^7.669 - t^7.688 + 9*t^7.734 + t^7.753 + 2*t^8.031 + 2*t^8.049 + 2*t^8.068 - t^8.114 - 6*t^8.133 + 3*t^8.198 + t^8.217 + t^8.457 + t^8.476 + 5*t^8.494 + 3*t^8.513 + 3*t^8.532 - t^8.559 - 11*t^8.578 - 3*t^8.597 + 2*t^8.662 + 2*t^8.875 + t^8.894 + 3*t^8.921 + 3*t^8.939 + t^8.958 + 4*t^8.977 - t^4.289/y - t^6.403/y - (2*t^6.867)/y + t^7.247/y + (3*t^7.692)/y + (5*t^7.711)/y + t^8.072/y + t^8.091/y + (4*t^8.156)/y + (2*t^8.175)/y - t^8.517/y + (3*t^8.536)/y + (3*t^8.62)/y + t^8.916/y + t^8.935/y - (2*t^8.981)/y - t^4.289*y - t^6.403*y - 2*t^6.867*y + t^7.247*y + 3*t^7.692*y + 5*t^7.711*y + t^8.072*y + t^8.091*y + 4*t^8.156*y + 2*t^8.175*y - t^8.517*y + 3*t^8.536*y + 3*t^8.62*y + t^8.916*y + t^8.935*y - 2*t^8.981*y (g2*t^2.114)/g1^5 + g1^3*g2^3*t^2.133 + (3*t^2.578)/(g1^2*g2^2) + (g2^5*t^2.958)/g1 + (g1*t^3.042)/g2^5 + g1^3*g2^9*t^3.802 + (g2^2*t^4.228)/g1^10 + (g2^4*t^4.247)/g1^2 + 2*g1^6*g2^6*t^4.266 + (3*t^4.692)/(g1^7*g2) + 4*g1*g2*t^4.711 + (g2^6*t^5.072)/g1^6 + g1^2*g2^8*t^5.091 + (6*t^5.156)/(g1^4*g2^4) + (g1^4*t^5.175)/g2^2 + (2*g2^3*t^5.536)/g1^3 + (2*t^5.62)/(g1*g2^7) + (2*g2^10*t^5.916)/g1^2 + g1^6*g2^12*t^5.935 - 3*t^6. + (g1^2*t^6.084)/g2^10 + (g2^3*t^6.343)/g1^15 + (g2^5*t^6.361)/g1^7 + 3*g1*g2^7*t^6.38 + 2*g1^9*g2^9*t^6.399 - t^6.445/(g1^5*g2^5) - (2*g1^3*t^6.464)/g2^3 + g1^2*g2^14*t^6.761 + (3*t^6.806)/g1^12 + (3*g2^2*t^6.825)/g1^4 + 4*g1^4*g2^4*t^6.844 - t^6.909/(g1^2*g2^8) + (g2^7*t^7.187)/g1^11 + (g2^9*t^7.205)/g1^3 + g1^5*g2^11*t^7.224 + (6*t^7.27)/(g1^9*g2^3) + (6*t^7.289)/(g1*g2) + g1^7*g2*t^7.308 + g1^6*g2^18*t^7.605 + (2*g2^4*t^7.65)/g1^8 + g2^6*t^7.669 - g1^8*g2^8*t^7.688 + (9*t^7.734)/(g1^6*g2^6) + (g1^2*t^7.753)/g2^4 + (2*g2^11*t^8.031)/g1^7 + 2*g1*g2^13*t^8.049 + 2*g1^9*g2^15*t^8.068 - (g2*t^8.114)/g1^5 - 6*g1^3*g2^3*t^8.133 + (3*t^8.198)/(g1^3*g2^9) + (g1^5*t^8.217)/g2^7 + (g2^4*t^8.457)/g1^20 + (g2^6*t^8.476)/g1^12 + (5*g2^8*t^8.494)/g1^4 + 3*g1^4*g2^10*t^8.513 + 3*g1^12*g2^12*t^8.532 - t^8.559/(g1^10*g2^4) - (11*t^8.578)/(g1^2*g2^2) - 3*g1^6*t^8.597 + (2*t^8.662)/g2^12 + (2*g2^15*t^8.875)/g1^3 + g1^5*g2^17*t^8.894 + (3*g2*t^8.921)/g1^17 + (3*g2^3*t^8.939)/g1^9 + (g2^5*t^8.958)/g1 + 4*g1^7*g2^7*t^8.977 - t^4.289/(g1*g2*y) - t^6.403/(g1^6*y) - (2*t^6.867)/(g1^3*g2^3*y) + (g2^4*t^7.247)/(g1^2*y) + (3*t^7.692)/(g1^7*g2*y) + (5*g1*g2*t^7.711)/y + (g2^6*t^8.072)/(g1^6*y) + (g1^2*g2^8*t^8.091)/y + (4*t^8.156)/(g1^4*g2^4*y) + (2*g1^4*t^8.175)/(g2^2*y) - (g2*t^8.517)/(g1^11*y) + (3*g2^3*t^8.536)/(g1^3*y) + (3*t^8.62)/(g1*g2^7*y) + (g2^10*t^8.916)/(g1^2*y) + (g1^6*g2^12*t^8.935)/y - (2*t^8.981)/(g1^8*g2^2*y) - (t^4.289*y)/(g1*g2) - (t^6.403*y)/g1^6 - (2*t^6.867*y)/(g1^3*g2^3) + (g2^4*t^7.247*y)/g1^2 + (3*t^7.692*y)/(g1^7*g2) + 5*g1*g2*t^7.711*y + (g2^6*t^8.072*y)/g1^6 + g1^2*g2^8*t^8.091*y + (4*t^8.156*y)/(g1^4*g2^4) + (2*g1^4*t^8.175*y)/g2^2 - (g2*t^8.517*y)/g1^11 + (3*g2^3*t^8.536*y)/g1^3 + (3*t^8.62*y)/(g1*g2^7) + (g2^10*t^8.916*y)/g1^2 + g1^6*g2^12*t^8.935*y - (2*t^8.981*y)/(g1^8*g2^2)


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
187 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ 0.5458 0.6894 0.7916 [M:[1.0, 1.0, 0.8656], q:[0.582, 0.9852], qb:[0.418, 0.2836], phi:[0.4328]] t^2.105 + 3*t^2.597 + 2*t^3. + 2*t^3.806 + 2*t^4.21 + 4*t^4.702 + 2*t^5.105 + 5*t^5.194 + 4*t^5.597 + 2*t^5.911 - t^6. - t^4.298/y - t^4.298*y detail