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
2083 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ 0.709 0.8787 0.8069 [M:[0.9142, 1.0286, 1.0858, 0.8571, 0.9142, 0.9142], q:[0.4571, 0.6286], qb:[0.4571, 0.5143], phi:[0.4857]] [M:[[-6], [2], [6], [-10], [-6], [-6]], q:[[-3], [9]], qb:[[-3], [1]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ ${}$ -4 t^2.571 + 3*t^2.743 + 2*t^2.914 + t^3.086 + 3*t^4.2 + 2*t^4.371 + t^4.543 + 2*t^4.714 + t^4.886 + t^5.142 + t^5.229 + 3*t^5.314 + 6*t^5.485 + 6*t^5.657 + 4*t^5.828 - 4*t^6. - 2*t^6.172 - t^6.343 - 2*t^6.515 + 3*t^6.771 + 9*t^6.943 + 10*t^7.114 + 6*t^7.286 + 2*t^7.457 + t^7.714 + 3*t^7.885 + 6*t^8.057 + 11*t^8.228 + 15*t^8.4 + 6*t^8.571 - 9*t^8.743 - 9*t^8.914 - t^4.457/y - t^7.028/y - (2*t^7.2)/y + (2*t^7.714)/y + t^7.886/y + (3*t^8.314)/y + (5*t^8.485)/y + (7*t^8.657)/y + (4*t^8.828)/y - t^4.457*y - t^7.028*y - 2*t^7.2*y + 2*t^7.714*y + t^7.886*y + 3*t^8.314*y + 5*t^8.485*y + 7*t^8.657*y + 4*t^8.828*y t^2.571/g1^10 + (3*t^2.743)/g1^6 + (2*t^2.914)/g1^2 + g1^2*t^3.086 + (3*t^4.2)/g1^7 + (2*t^4.371)/g1^3 + g1*t^4.543 + 2*g1^5*t^4.714 + g1^9*t^4.886 + t^5.142/g1^20 + g1^17*t^5.229 + (3*t^5.314)/g1^16 + (6*t^5.485)/g1^12 + (6*t^5.657)/g1^8 + (4*t^5.828)/g1^4 - 4*t^6. - 2*g1^4*t^6.172 - g1^8*t^6.343 - 2*g1^12*t^6.515 + (3*t^6.771)/g1^17 + (9*t^6.943)/g1^13 + (10*t^7.114)/g1^9 + (6*t^7.286)/g1^5 + (2*t^7.457)/g1 + t^7.714/g1^30 + (3*t^7.885)/g1^26 + (6*t^8.057)/g1^22 + (11*t^8.228)/g1^18 + (15*t^8.4)/g1^14 + (6*t^8.571)/g1^10 - (9*t^8.743)/g1^6 - (9*t^8.914)/g1^2 - t^4.457/(g1*y) - t^7.028/(g1^11*y) - (2*t^7.2)/(g1^7*y) + (2*g1^5*t^7.714)/y + (g1^9*t^7.886)/y + (3*t^8.314)/(g1^16*y) + (5*t^8.485)/(g1^12*y) + (7*t^8.657)/(g1^8*y) + (4*t^8.828)/(g1^4*y) - (t^4.457*y)/g1 - (t^7.028*y)/g1^11 - (2*t^7.2*y)/g1^7 + 2*g1^5*t^7.714*y + g1^9*t^7.886*y + (3*t^8.314*y)/g1^16 + (5*t^8.485*y)/g1^12 + (7*t^8.657*y)/g1^8 + (4*t^8.828*y)/g1^4


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
899 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ 0.702 0.8645 0.812 [M:[0.933, 1.0223, 1.067, 0.8883, 0.933], q:[0.4665, 0.6005], qb:[0.4665, 0.5112], phi:[0.4888]] t^2.665 + 2*t^2.799 + 2*t^2.933 + t^3.067 + t^3.201 + 3*t^4.265 + 2*t^4.399 + t^4.534 + 2*t^4.668 + t^4.802 + t^5.07 + t^5.33 + 2*t^5.464 + 3*t^5.598 + 4*t^5.732 + 4*t^5.866 - 2*t^6. - t^4.466/y - t^4.466*y detail