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
1854 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ 0.5415 0.6866 0.7886 [M:[1.023, 0.977, 1.1494, 0.977, 0.6781], q:[0.5517, 1.023], qb:[0.4253, 0.2989], phi:[0.4253]] [M:[[7], [-7], [2], [-7], [-11]], q:[[-6], [7]], qb:[[-1], [4]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ ${}M_{3}q_{1}\tilde{q}_{2}$ -1 t^2.034 + t^2.172 + t^2.552 + 2*t^2.931 + 2*t^3.448 + t^3.828 + t^4.069 + t^4.207 + 2*t^4.345 + t^4.586 + 2*t^4.724 + 2*t^4.965 + 2*t^5.103 + 3*t^5.483 + t^5.621 + 4*t^5.862 - t^6. + t^6.103 + t^6.241 + 4*t^6.379 + t^6.62 + 3*t^6.758 + t^6.897 + 2*t^6.999 + 2*t^7.138 + 3*t^7.276 - t^7.414 + 3*t^7.517 + 3*t^7.655 + 4*t^7.896 + t^8.034 + t^8.137 - 2*t^8.172 + t^8.275 + 5*t^8.413 - t^8.552 + t^8.655 + 7*t^8.793 - 4*t^8.931 - t^4.276/y - t^6.31/y + t^7.345/y + t^7.586/y + t^7.724/y + (2*t^7.965)/y + (2*t^8.103)/y + t^8.242/y - t^8.344/y + (4*t^8.483)/y + (2*t^8.621)/y + (2*t^8.862)/y - t^4.276*y - t^6.31*y + t^7.345*y + t^7.586*y + t^7.724*y + 2*t^7.965*y + 2*t^8.103*y + t^8.242*y - t^8.344*y + 4*t^8.483*y + 2*t^8.621*y + 2*t^8.862*y t^2.034/g1^11 + g1^3*t^2.172 + t^2.552/g1^2 + (2*t^2.931)/g1^7 + 2*g1^2*t^3.448 + t^3.828/g1^3 + t^4.069/g1^22 + t^4.207/g1^8 + 2*g1^6*t^4.345 + t^4.586/g1^13 + 2*g1*t^4.724 + (2*t^4.965)/g1^18 + (2*t^5.103)/g1^4 + (3*t^5.483)/g1^9 + g1^5*t^5.621 + (4*t^5.862)/g1^14 - t^6. + t^6.103/g1^33 + t^6.241/g1^19 + (4*t^6.379)/g1^5 + t^6.62/g1^24 + (3*t^6.758)/g1^10 + g1^4*t^6.897 + (2*t^6.999)/g1^29 + (2*t^7.138)/g1^15 + (3*t^7.276)/g1 - g1^13*t^7.414 + (3*t^7.517)/g1^20 + (3*t^7.655)/g1^6 + (4*t^7.896)/g1^25 + t^8.034/g1^11 + t^8.137/g1^44 - 2*g1^3*t^8.172 + t^8.275/g1^30 + (5*t^8.413)/g1^16 - t^8.552/g1^2 + t^8.655/g1^35 + (7*t^8.793)/g1^21 - (4*t^8.931)/g1^7 - t^4.276/(g1*y) - t^6.31/(g1^12*y) + (g1^6*t^7.345)/y + t^7.586/(g1^13*y) + (g1*t^7.724)/y + (2*t^7.965)/(g1^18*y) + (2*t^8.103)/(g1^4*y) + (g1^10*t^8.242)/y - t^8.344/(g1^23*y) + (4*t^8.483)/(g1^9*y) + (2*g1^5*t^8.621)/y + (2*t^8.862)/(g1^14*y) - (t^4.276*y)/g1 - (t^6.31*y)/g1^12 + g1^6*t^7.345*y + (t^7.586*y)/g1^13 + g1*t^7.724*y + (2*t^7.965*y)/g1^18 + (2*t^8.103*y)/g1^4 + g1^10*t^8.242*y - (t^8.344*y)/g1^23 + (4*t^8.483*y)/g1^9 + 2*g1^5*t^8.621*y + (2*t^8.862*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
466 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{1}M_{4}$ 0.5207 0.6457 0.8064 [M:[1.0179, 0.9821, 1.148, 0.9821], q:[0.5561, 1.0179], qb:[0.426, 0.2959], phi:[0.426]] t^2.166 + t^2.556 + 2*t^2.946 + 2*t^3.444 + t^3.834 + t^3.941 + 2*t^4.332 + 2*t^4.722 + 2*t^5.112 + t^5.502 + t^5.61 + 3*t^5.893 - t^6. - t^4.278/y - t^4.278*y detail