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
56547 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}M_{7}$ 0.675 0.8455 0.7983 [M:[1.1651, 1.068, 0.8349, 0.7961, 0.699, 1.2039, 0.8349], q:[0.3981, 0.4369], qb:[0.534, 0.767], phi:[0.466]] [M:[[-5], [4], [5], [-12], [-3], [12], [5]], q:[[-6], [11]], qb:[[2], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }M_{3}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{7}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ ${}M_{5}\tilde{q}_{1}\tilde{q}_{2}$ -1 t^2.097 + 2*t^2.505 + t^2.796 + t^2.913 + t^3.204 + t^3.612 + t^3.786 + t^3.903 + t^4.019 + 2*t^4.194 + t^4.311 + 3*t^4.602 + t^4.893 + 4*t^5.01 + 3*t^5.301 + 2*t^5.417 + 3*t^5.709 + t^5.825 - t^6. + 3*t^6.116 + 2*t^6.291 + 2*t^6.408 + 3*t^6.524 + t^6.583 + 4*t^6.699 + 4*t^6.815 + t^6.932 + 5*t^7.107 + 2*t^7.223 - t^7.282 + 2*t^7.398 + 6*t^7.515 + t^7.573 + t^7.631 - t^7.689 + 5*t^7.806 + 5*t^7.922 + t^7.981 + t^8.039 - 2*t^8.097 + 6*t^8.214 + 3*t^8.33 + t^8.388 - 3*t^8.505 + 7*t^8.621 + t^8.738 + t^8.796 + 2*t^8.913 - t^4.398/y - t^6.495/y - t^6.903/y + (2*t^7.602)/y + (2*t^7.893)/y + (2*t^8.01)/y + (4*t^8.301)/y + (2*t^8.417)/y - t^8.592/y + (4*t^8.709)/y + t^8.884/y - t^4.398*y - t^6.495*y - t^6.903*y + 2*t^7.602*y + 2*t^7.893*y + 2*t^8.01*y + 4*t^8.301*y + 2*t^8.417*y - t^8.592*y + 4*t^8.709*y + t^8.884*y t^2.097/g1^3 + 2*g1^5*t^2.505 + t^2.796/g1^4 + g1^13*t^2.913 + g1^4*t^3.204 + g1^12*t^3.612 + t^3.786/g1^14 + g1^3*t^3.903 + g1^20*t^4.019 + (2*t^4.194)/g1^6 + g1^11*t^4.311 + 3*g1^2*t^4.602 + t^4.893/g1^7 + 4*g1^10*t^5.01 + 3*g1*t^5.301 + 2*g1^18*t^5.417 + 3*g1^9*t^5.709 + g1^26*t^5.825 - t^6. + 3*g1^17*t^6.116 + (2*t^6.291)/g1^9 + 2*g1^8*t^6.408 + 3*g1^25*t^6.524 + t^6.583/g1^18 + (4*t^6.699)/g1 + 4*g1^16*t^6.815 + g1^33*t^6.932 + 5*g1^7*t^7.107 + 2*g1^24*t^7.223 - t^7.282/g1^19 + (2*t^7.398)/g1^2 + 6*g1^15*t^7.515 + t^7.573/g1^28 + g1^32*t^7.631 - t^7.689/g1^11 + 5*g1^6*t^7.806 + 5*g1^23*t^7.922 + t^7.981/g1^20 + g1^40*t^8.039 - (2*t^8.097)/g1^3 + 6*g1^14*t^8.214 + 3*g1^31*t^8.33 + t^8.388/g1^12 - 3*g1^5*t^8.505 + 7*g1^22*t^8.621 + g1^39*t^8.738 + t^8.796/g1^4 + 2*g1^13*t^8.913 - t^4.398/(g1^2*y) - t^6.495/(g1^5*y) - (g1^3*t^6.903)/y + (2*g1^2*t^7.602)/y + (2*t^7.893)/(g1^7*y) + (2*g1^10*t^8.01)/y + (4*g1*t^8.301)/y + (2*g1^18*t^8.417)/y - t^8.592/(g1^8*y) + (4*g1^9*t^8.709)/y + t^8.884/(g1^17*y) - (t^4.398*y)/g1^2 - (t^6.495*y)/g1^5 - g1^3*t^6.903*y + 2*g1^2*t^7.602*y + (2*t^7.893*y)/g1^7 + 2*g1^10*t^8.01*y + 4*g1*t^8.301*y + 2*g1^18*t^8.417*y - (t^8.592*y)/g1^8 + 4*g1^9*t^8.709*y + (t^8.884*y)/g1^17


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
53796 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}M_{6}$ 0.661 0.8205 0.8057 [M:[1.1596, 1.0724, 0.8404, 0.7829, 0.6957, 1.2171], q:[0.3915, 0.449], qb:[0.5362, 0.7681], phi:[0.4638]] t^2.087 + t^2.521 + t^2.783 + t^2.955 + t^3.217 + t^3.479 + t^3.651 + t^3.74 + t^3.913 + t^4.085 + 2*t^4.174 + t^4.347 + 2*t^4.609 + t^4.87 + 2*t^5.043 + 2*t^5.304 + t^5.477 + t^5.566 + 2*t^5.738 + t^5.911 - t^4.391/y - t^4.391*y detail