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
1359 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{6}$ 0.5972 0.7561 0.7898 [M:[1.0, 0.8308, 0.7115, 0.7462, 1.1692, 1.2885], q:[0.7712, 0.2288], qb:[0.6019, 0.5673], phi:[0.4577]] [M:[[0], [-8], [10], [-12], [8], [-10]], q:[[1], [-1]], qb:[[-7], [15]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{5}$, ${ }M_{1}\phi_{1}^{2}$ ${}$ -2 t^2.239 + t^2.388 + t^2.492 + 2*t^2.746 + t^3. + t^3.508 + t^3.865 + t^4.015 + t^4.119 + t^4.477 + t^4.627 + t^4.731 + 2*t^4.777 + t^4.881 + 3*t^4.985 + 2*t^5.135 + 3*t^5.239 + t^5.388 + 4*t^5.492 + 2*t^5.746 - 2*t^6. + 2*t^6.254 + t^6.358 + t^6.404 + t^6.508 + 2*t^6.612 + t^6.716 + 2*t^6.865 + t^6.97 + 2*t^7.015 + 2*t^7.165 + 3*t^7.223 + t^7.373 + 3*t^7.477 + 4*t^7.523 + t^7.627 + 6*t^7.731 + t^7.777 + 3*t^7.881 + 6*t^7.985 + t^8.135 + 3*t^8.239 + t^8.284 - 3*t^8.388 + t^8.596 - 6*t^8.746 + 2*t^8.792 + t^8.85 + t^8.896 + t^8.954 - t^4.373/y - t^6.612/y - t^7.119/y + (2*t^7.627)/y + t^7.731/y + t^7.881/y + (2*t^7.985)/y + (3*t^8.135)/y + (3*t^8.239)/y + t^8.388/y + (2*t^8.492)/y + (3*t^8.746)/y - t^8.85/y + t^8.896/y - t^4.373*y - t^6.612*y - t^7.119*y + 2*t^7.627*y + t^7.731*y + t^7.881*y + 2*t^7.985*y + 3*t^8.135*y + 3*t^8.239*y + t^8.388*y + 2*t^8.492*y + 3*t^8.746*y - t^8.85*y + t^8.896*y t^2.239/g1^12 + g1^14*t^2.388 + t^2.492/g1^8 + (2*t^2.746)/g1^4 + t^3. + g1^8*t^3.508 + t^3.865/g1^10 + g1^16*t^4.015 + t^4.119/g1^6 + t^4.477/g1^24 + g1^2*t^4.627 + t^4.731/g1^20 + 2*g1^28*t^4.777 + g1^6*t^4.881 + (3*t^4.985)/g1^16 + 2*g1^10*t^5.135 + (3*t^5.239)/g1^12 + g1^14*t^5.388 + (4*t^5.492)/g1^8 + (2*t^5.746)/g1^4 - 2*t^6. + 2*g1^4*t^6.254 + t^6.358/g1^18 + g1^30*t^6.404 + g1^8*t^6.508 + (2*t^6.612)/g1^14 + t^6.716/g1^36 + (2*t^6.865)/g1^10 + t^6.97/g1^32 + 2*g1^16*t^7.015 + 2*g1^42*t^7.165 + (3*t^7.223)/g1^28 + t^7.373/g1^2 + (3*t^7.477)/g1^24 + 4*g1^24*t^7.523 + g1^2*t^7.627 + (6*t^7.731)/g1^20 + g1^28*t^7.777 + 3*g1^6*t^7.881 + (6*t^7.985)/g1^16 + g1^10*t^8.135 + (3*t^8.239)/g1^12 + g1^36*t^8.284 - 3*g1^14*t^8.388 + t^8.596/g1^30 - (6*t^8.746)/g1^4 + 2*g1^44*t^8.792 + t^8.85/g1^26 + g1^22*t^8.896 + t^8.954/g1^48 - t^4.373/(g1^2*y) - t^6.612/(g1^14*y) - t^7.119/(g1^6*y) + (2*g1^2*t^7.627)/y + t^7.731/(g1^20*y) + (g1^6*t^7.881)/y + (2*t^7.985)/(g1^16*y) + (3*g1^10*t^8.135)/y + (3*t^8.239)/(g1^12*y) + (g1^14*t^8.388)/y + (2*t^8.492)/(g1^8*y) + (3*t^8.746)/(g1^4*y) - t^8.85/(g1^26*y) + (g1^22*t^8.896)/y - (t^4.373*y)/g1^2 - (t^6.612*y)/g1^14 - (t^7.119*y)/g1^6 + 2*g1^2*t^7.627*y + (t^7.731*y)/g1^20 + g1^6*t^7.881*y + (2*t^7.985*y)/g1^16 + 3*g1^10*t^8.135*y + (3*t^8.239*y)/g1^12 + g1^14*t^8.388*y + (2*t^8.492*y)/g1^8 + (3*t^8.746*y)/g1^4 - (t^8.85*y)/g1^26 + g1^22*t^8.896*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


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
867 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ 0.6175 0.7947 0.7771 [M:[1.0, 0.8344, 0.707, 0.7516, 1.1656], q:[0.7707, 0.2293], qb:[0.6051, 0.5605], phi:[0.4586]] t^2.121 + t^2.255 + t^2.369 + t^2.503 + 2*t^2.752 + t^3. + t^3.497 + t^3.994 + t^4.127 + t^4.242 + t^4.376 + t^4.49 + t^4.51 + 2*t^4.624 + 2*t^4.739 + t^4.758 + 3*t^4.873 + 3*t^5.006 + 3*t^5.121 + 3*t^5.255 + t^5.369 + 4*t^5.503 + t^5.618 + 2*t^5.752 - 2*t^6. - t^4.376/y - t^4.376*y detail