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
56115 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{7}\phi_{1}q_{1}q_{2}$ 0.6419 0.804 0.7983 [X:[1.4049], M:[1.0951, 1.0246, 0.9049, 0.5951, 1.0, 0.7148, 0.6901], q:[0.2975, 0.6074], qb:[0.6778, 0.7975], phi:[0.4049]] [X:[[2]], M:[[-2], [10], [2], [-2], [0], [6], [-4]], q:[[-1], [3]], qb:[[-9], [-1]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{7}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{2}$, ${ }M_{1}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}M_{7}$, ${ }X_{1}$, ${ }M_{6}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{1}\phi_{1}^{2}$ ${}$ -1 t^2.07 + t^2.144 + t^2.43 + t^2.715 + t^3. + t^3.074 + t^3.285 + 2*t^4.141 + 2*t^4.215 + t^4.289 + t^4.426 + t^4.5 + t^4.574 + t^4.785 + 2*t^4.859 + t^5.07 + 3*t^5.144 + t^5.218 + t^5.282 + t^5.356 + 3*t^5.43 + t^5.504 + t^5.715 - t^6. + t^6.148 + t^6.211 + 3*t^6.285 + 2*t^6.359 + t^6.433 + t^6.496 + 2*t^6.57 + t^6.644 + t^6.718 + t^6.856 + 2*t^6.93 + t^7.004 + t^7.141 + 2*t^7.215 + 5*t^7.289 + t^7.352 + t^7.363 + 2*t^7.426 + 3*t^7.5 + 5*t^7.574 + t^7.648 + t^7.711 + 2*t^7.859 + 2*t^7.933 - 3*t^8.07 + t^8.218 + 2*t^8.282 + t^8.292 + 2*t^8.356 + 2*t^8.43 + 2*t^8.504 + 2*t^8.567 + 2*t^8.577 + t^8.641 + t^8.789 + t^8.863 - t^4.215/y - t^6.285/y - t^6.359/y - t^6.644/y + t^7.141/y + t^7.215/y - t^7.289/y + t^7.5/y + t^7.574/y + (2*t^7.785)/y + t^7.859/y + (2*t^8.07)/y + (4*t^8.144)/y + t^8.218/y + t^8.43/y + t^8.715/y - t^4.215*y - t^6.285*y - t^6.359*y - t^6.644*y + t^7.141*y + t^7.215*y - t^7.289*y + t^7.5*y + t^7.574*y + 2*t^7.785*y + t^7.859*y + 2*t^8.07*y + 4*t^8.144*y + t^8.218*y + t^8.43*y + t^8.715*y t^2.07/g1^4 + g1^6*t^2.144 + g1^4*t^2.43 + g1^2*t^2.715 + t^3. + g1^10*t^3.074 + t^3.285/g1^2 + (2*t^4.141)/g1^8 + 2*g1^2*t^4.215 + g1^12*t^4.289 + t^4.426/g1^10 + t^4.5 + g1^10*t^4.574 + t^4.785/g1^2 + 2*g1^8*t^4.859 + t^5.07/g1^4 + 3*g1^6*t^5.144 + g1^16*t^5.218 + t^5.282/g1^16 + t^5.356/g1^6 + 3*g1^4*t^5.43 + g1^14*t^5.504 + g1^2*t^5.715 - t^6. + g1^20*t^6.148 + t^6.211/g1^12 + (3*t^6.285)/g1^2 + 2*g1^8*t^6.359 + g1^18*t^6.433 + t^6.496/g1^14 + (2*t^6.57)/g1^4 + g1^6*t^6.644 + g1^16*t^6.718 + t^6.856/g1^6 + 2*g1^4*t^6.93 + g1^14*t^7.004 + t^7.141/g1^8 + 2*g1^2*t^7.215 + 5*g1^12*t^7.289 + t^7.352/g1^20 + g1^22*t^7.363 + (2*t^7.426)/g1^10 + 3*t^7.5 + 5*g1^10*t^7.574 + g1^20*t^7.648 + t^7.711/g1^12 + 2*g1^8*t^7.859 + 2*g1^18*t^7.933 - (3*t^8.07)/g1^4 + g1^16*t^8.218 + (2*t^8.282)/g1^16 + g1^26*t^8.292 + (2*t^8.356)/g1^6 + 2*g1^4*t^8.43 + 2*g1^14*t^8.504 + (2*t^8.567)/g1^18 + 2*g1^24*t^8.577 + t^8.641/g1^8 + g1^12*t^8.789 + g1^22*t^8.863 - (g1^2*t^4.215)/y - t^6.285/(g1^2*y) - (g1^8*t^6.359)/y - (g1^6*t^6.644)/y + t^7.141/(g1^8*y) + (g1^2*t^7.215)/y - (g1^12*t^7.289)/y + t^7.5/y + (g1^10*t^7.574)/y + (2*t^7.785)/(g1^2*y) + (g1^8*t^7.859)/y + (2*t^8.07)/(g1^4*y) + (4*g1^6*t^8.144)/y + (g1^16*t^8.218)/y + (g1^4*t^8.43)/y + (g1^2*t^8.715)/y - g1^2*t^4.215*y - (t^6.285*y)/g1^2 - g1^8*t^6.359*y - g1^6*t^6.644*y + (t^7.141*y)/g1^8 + g1^2*t^7.215*y - g1^12*t^7.289*y + t^7.5*y + g1^10*t^7.574*y + (2*t^7.785*y)/g1^2 + g1^8*t^7.859*y + (2*t^8.07*y)/g1^4 + 4*g1^6*t^8.144*y + g1^16*t^8.218*y + g1^4*t^8.43*y + g1^2*t^8.715*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
50836 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{4}X_{1}$ 0.6212 0.7642 0.8129 [X:[1.4041], M:[1.0959, 1.0207, 0.9041, 0.5959, 1.0, 0.7124], q:[0.2979, 0.6062], qb:[0.6814, 0.7979], phi:[0.4041]] t^2.137 + t^2.425 + t^2.712 + t^3. + t^3.062 + t^3.288 + t^3.925 + t^4.15 + t^4.212 + t^4.274 + t^4.438 + t^4.562 + 2*t^4.85 + 2*t^5.137 + t^5.199 + t^5.301 + 3*t^5.425 + t^5.487 + t^5.712 - t^6. - t^4.212/y - t^4.212*y detail