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
46557 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ 0.5418 0.6877 0.7879 [M:[0.8669, 1.1331, 1.1331, 0.6997], q:[0.9659, 0.6007], qb:[0.2662, 0.4334], phi:[0.4334]] [M:[[2], [-2], [-2], [-3]], q:[[-7], [6]], qb:[[-4], [1]], phi:[[1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{4}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ ${}M_{3}\phi_{1}^{2}$ -1 2*t^2.099 + t^2.601 + t^2.898 + t^3.102 + 2*t^3.399 + t^3.696 + 4*t^4.198 + 3*t^4.7 + 2*t^4.997 + 2*t^5.201 + 4*t^5.498 + 3*t^5.795 - t^6. + t^6.205 + 7*t^6.297 - t^6.502 + t^6.594 + 5*t^6.799 - t^7.003 + 5*t^7.096 + t^7.3 + t^7.393 + 6*t^7.597 - t^7.802 + 6*t^7.894 - 4*t^8.099 + t^8.304 + 11*t^8.396 - 5*t^8.601 + 3*t^8.693 + 4*t^8.898 - t^4.3/y - t^6.399/y + t^7.198/y + (2*t^7.7)/y + (2*t^7.997)/y + (3*t^8.201)/y + (4*t^8.498)/y + t^8.703/y + (2*t^8.795)/y - t^4.3*y - t^6.399*y + t^7.198*y + 2*t^7.7*y + 2*t^7.997*y + 3*t^8.201*y + 4*t^8.498*y + t^8.703*y + 2*t^8.795*y (2*t^2.099)/g1^3 + g1^2*t^2.601 + t^2.898/g1^7 + g1^7*t^3.102 + (2*t^3.399)/g1^2 + t^3.696/g1^11 + (4*t^4.198)/g1^6 + (3*t^4.7)/g1 + (2*t^4.997)/g1^10 + 2*g1^4*t^5.201 + (4*t^5.498)/g1^5 + (3*t^5.795)/g1^14 - t^6. + g1^14*t^6.205 + (7*t^6.297)/g1^9 - g1^5*t^6.502 + t^6.594/g1^18 + (5*t^6.799)/g1^4 - g1^10*t^7.003 + (5*t^7.096)/g1^13 + g1*t^7.3 + t^7.393/g1^22 + (6*t^7.597)/g1^8 - g1^6*t^7.802 + (6*t^7.894)/g1^17 - (4*t^8.099)/g1^3 + g1^11*t^8.304 + (11*t^8.396)/g1^12 - 5*g1^2*t^8.601 + (3*t^8.693)/g1^21 + (4*t^8.898)/g1^7 - (g1*t^4.3)/y - t^6.399/(g1^2*y) + t^7.198/(g1^6*y) + (2*t^7.7)/(g1*y) + (2*t^7.997)/(g1^10*y) + (3*g1^4*t^8.201)/y + (4*t^8.498)/(g1^5*y) + (g1^9*t^8.703)/y + (2*t^8.795)/(g1^14*y) - g1*t^4.3*y - (t^6.399*y)/g1^2 + (t^7.198*y)/g1^6 + (2*t^7.7*y)/g1 + (2*t^7.997*y)/g1^10 + 3*g1^4*t^8.201*y + (4*t^8.498*y)/g1^5 + g1^9*t^8.703*y + (2*t^8.795*y)/g1^14


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
46151 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ + ${ }M_{1}M_{3}$ 0.5213 0.6482 0.8042 [M:[0.8658, 1.1342, 1.1342], q:[0.9697, 0.5974], qb:[0.2684, 0.4329], phi:[0.4329]] t^2.104 + t^2.597 + t^2.909 + t^3.091 + 2*t^3.403 + t^3.714 + t^3.896 + 2*t^4.208 + 2*t^4.701 + t^5.013 + t^5.195 + 2*t^5.506 + 2*t^5.818 - t^4.299/y - t^4.299*y detail {a: 148361/284592, c: 92237/142296, M1: 200/231, M2: 262/231, M3: 262/231, q1: 32/33, q2: 46/77, qb1: 62/231, qb2: 100/231, phi1: 100/231}