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
46082 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ 0.6324 0.8242 0.7672 [M:[0.9651, 0.7413, 0.811], q:[0.7413, 0.2936], qb:[0.4477, 0.4477], phi:[0.5174]] [M:[[4], [1], [-7]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ 0 3*t^2.224 + t^2.433 + t^2.686 + t^2.895 + t^3.105 + t^3.314 + t^3.567 + t^3.776 + 3*t^4.239 + 6*t^4.448 + 3*t^4.657 + t^4.866 + 3*t^4.91 + 4*t^5.119 + 4*t^5.328 + t^5.372 + 2*t^5.538 + t^5.582 + t^5.747 + 4*t^5.791 + t^6.209 + t^6.253 + t^6.418 + 7*t^6.462 + t^6.628 + 11*t^6.672 + 4*t^6.881 + 3*t^6.925 + 2*t^7.09 + 7*t^7.134 + t^7.299 + 8*t^7.343 + 6*t^7.552 + 3*t^7.596 + 4*t^7.761 + 5*t^7.805 + 2*t^7.971 + 7*t^8.015 + t^8.059 + t^8.18 - 4*t^8.224 + t^8.268 - 2*t^8.433 + 9*t^8.477 + 2*t^8.642 + 9*t^8.686 + 2*t^8.851 + 11*t^8.895 + t^8.939 - t^4.552/y - t^6.776/y - t^6.985/y + (3*t^7.448)/y + (3*t^7.657)/y + (3*t^7.91)/y + (5*t^8.119)/y + (5*t^8.328)/y + (4*t^8.538)/y + t^8.582/y + t^8.747/y + (4*t^8.791)/y - t^4.552*y - t^6.776*y - t^6.985*y + 3*t^7.448*y + 3*t^7.657*y + 3*t^7.91*y + 5*t^8.119*y + 5*t^8.328*y + 4*t^8.538*y + t^8.582*y + t^8.747*y + 4*t^8.791*y 3*g1*t^2.224 + t^2.433/g1^7 + g1^12*t^2.686 + g1^4*t^2.895 + t^3.105/g1^4 + t^3.314/g1^12 + g1^7*t^3.567 + t^3.776/g1 + 3*g1^10*t^4.239 + 6*g1^2*t^4.448 + (3*t^4.657)/g1^6 + t^4.866/g1^14 + 3*g1^13*t^4.91 + 4*g1^5*t^5.119 + (4*t^5.328)/g1^3 + g1^24*t^5.372 + (2*t^5.538)/g1^11 + g1^16*t^5.582 + t^5.747/g1^19 + 4*g1^8*t^5.791 + t^6.209/g1^8 + g1^19*t^6.253 + t^6.418/g1^16 + 7*g1^11*t^6.462 + t^6.628/g1^24 + 11*g1^3*t^6.672 + (4*t^6.881)/g1^5 + 3*g1^22*t^6.925 + (2*t^7.09)/g1^13 + 7*g1^14*t^7.134 + t^7.299/g1^21 + 8*g1^6*t^7.343 + (6*t^7.552)/g1^2 + 3*g1^25*t^7.596 + (4*t^7.761)/g1^10 + 5*g1^17*t^7.805 + (2*t^7.971)/g1^18 + 7*g1^9*t^8.015 + g1^36*t^8.059 + t^8.18/g1^26 - 4*g1*t^8.224 + g1^28*t^8.268 - (2*t^8.433)/g1^7 + 9*g1^20*t^8.477 + (2*t^8.642)/g1^15 + 9*g1^12*t^8.686 + (2*t^8.851)/g1^23 + 11*g1^4*t^8.895 + g1^31*t^8.939 - t^4.552/(g1^2*y) - t^6.776/(g1*y) - t^6.985/(g1^9*y) + (3*g1^2*t^7.448)/y + (3*t^7.657)/(g1^6*y) + (3*g1^13*t^7.91)/y + (5*g1^5*t^8.119)/y + (5*t^8.328)/(g1^3*y) + (4*t^8.538)/(g1^11*y) + (g1^16*t^8.582)/y + t^8.747/(g1^19*y) + (4*g1^8*t^8.791)/y - (t^4.552*y)/g1^2 - (t^6.776*y)/g1 - (t^6.985*y)/g1^9 + 3*g1^2*t^7.448*y + (3*t^7.657*y)/g1^6 + 3*g1^13*t^7.91*y + 5*g1^5*t^8.119*y + (5*t^8.328*y)/g1^3 + (4*t^8.538*y)/g1^11 + g1^16*t^8.582*y + (t^8.747*y)/g1^19 + 4*g1^8*t^8.791*y


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
46571 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ 0.6518 0.8599 0.758 [M:[0.9645, 0.7411, 0.8122, 0.7411], q:[0.7411, 0.2944], qb:[0.4467, 0.4467], phi:[0.5178]] 4*t^2.223 + t^2.437 + t^2.68 + t^2.893 + t^3.107 + t^3.32 + t^3.563 + 3*t^4.233 + 10*t^4.447 + 4*t^4.66 + t^4.873 + 4*t^4.904 + 5*t^5.117 + 5*t^5.33 + t^5.36 + 3*t^5.543 + t^5.574 + t^5.756 + 5*t^5.787 - 3*t^6. - t^4.553/y - t^4.553*y detail
46390 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ 0.6359 0.8312 0.7651 [M:[0.9585, 0.7396, 0.8227, 0.9585], q:[0.7396, 0.3019], qb:[0.4377, 0.4377], phi:[0.5208]] 3*t^2.219 + t^2.468 + t^2.626 + 2*t^2.875 + t^3.374 + t^3.532 + t^3.781 + 3*t^4.189 + 6*t^4.438 + 3*t^4.687 + 3*t^4.845 + t^4.936 + 7*t^5.094 + t^5.253 + 2*t^5.343 + 2*t^5.502 + t^5.593 + 5*t^5.751 + t^5.842 - t^6. - t^4.562/y - t^4.562*y detail


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
46044 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ 0.6335 0.8282 0.7649 [M:[0.9646, 0.7188, 0.7897], q:[0.7411, 0.2943], qb:[0.4692, 0.4245], phi:[0.5177]] 2*t^2.156 + t^2.29 + t^2.369 + t^2.681 + t^2.894 + t^3.106 + t^3.319 + t^3.497 + t^3.71 + t^4.1 + t^4.234 + 3*t^4.313 + t^4.368 + 2*t^4.447 + 2*t^4.525 + t^4.581 + t^4.66 + t^4.738 + 2*t^4.837 + t^4.971 + 3*t^5.05 + t^5.184 + 3*t^5.263 + t^5.362 + t^5.397 + 2*t^5.475 + t^5.575 + 2*t^5.653 + t^5.688 + 2*t^5.787 + 2*t^5.866 - t^6. - t^4.553/y - t^4.553*y detail