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
56302 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}^{2}$ + ${ }M_{7}q_{2}\tilde{q}_{1}$ 0.595 0.7426 0.8012 [M:[1.2286, 0.6859, 0.7714, 0.9523, 1.1809, 1.0, 0.8668], q:[0.4761, 0.2952], qb:[0.8379, 0.7525], phi:[0.4095]] [M:[[6], [18], [-6], [-10], [-4], [0], [14]], q:[[-5], [-1]], qb:[[-13], [11]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{3}$, ${ }M_{7}$, ${ }M_{4}$, ${ }M_{6}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{7}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{7}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{2}M_{5}$, ${ }M_{6}M_{7}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{6}$ ${}$ -1 t^2.058 + t^2.314 + t^2.6 + t^2.857 + t^3. + 2*t^3.543 + t^3.686 + t^4.085 + t^4.116 + t^4.372 + t^4.628 + t^4.658 + t^4.771 + 2*t^4.915 + t^5.058 + t^5.171 + t^5.201 + t^5.314 + 2*t^5.6 + t^5.714 + t^5.744 + 2*t^5.857 - t^6. + 2*t^6.143 + t^6.173 + t^6.286 + 2*t^6.4 + t^6.43 + t^6.543 + t^6.686 + t^6.716 + t^6.942 + 2*t^6.972 + t^7.085 + t^7.116 + t^7.229 + t^7.259 + 2*t^7.372 + t^7.515 + 2*t^7.628 + 2*t^7.658 + t^7.771 + 2*t^7.801 + t^7.915 + t^8.028 - t^8.058 + 2*t^8.171 + 2*t^8.201 + t^8.231 - t^8.314 + t^8.344 + 2*t^8.457 + t^8.487 + t^8.57 - t^8.6 + t^8.714 + 2*t^8.744 + t^8.774 - 2*t^8.857 + t^8.887 - t^4.229/y - t^6.286/y - t^6.829/y - t^7.085/y + (2*t^7.372)/y + t^7.628/y + t^7.658/y + (2*t^7.915)/y + t^8.058/y + (2*t^8.171)/y + t^8.314/y - t^8.344/y + t^8.457/y + (3*t^8.6)/y + t^8.744/y + (3*t^8.857)/y - t^8.887/y - t^4.229*y - t^6.286*y - t^6.829*y - t^7.085*y + 2*t^7.372*y + t^7.628*y + t^7.658*y + 2*t^7.915*y + t^8.058*y + 2*t^8.171*y + t^8.314*y - t^8.344*y + t^8.457*y + 3*t^8.6*y + t^8.744*y + 3*t^8.857*y - t^8.887*y g1^18*t^2.058 + t^2.314/g1^6 + g1^14*t^2.6 + t^2.857/g1^10 + t^3. + (2*t^3.543)/g1^4 + g1^6*t^3.686 + t^4.085/g1^8 + g1^36*t^4.116 + g1^12*t^4.372 + t^4.628/g1^12 + g1^32*t^4.658 + t^4.771/g1^2 + 2*g1^8*t^4.915 + g1^18*t^5.058 + t^5.171/g1^16 + g1^28*t^5.201 + t^5.314/g1^6 + 2*g1^14*t^5.6 + t^5.714/g1^20 + g1^24*t^5.744 + (2*t^5.857)/g1^10 - t^6. + 2*g1^10*t^6.143 + g1^54*t^6.173 + g1^20*t^6.286 + (2*t^6.4)/g1^14 + g1^30*t^6.43 + t^6.543/g1^4 + g1^6*t^6.686 + g1^50*t^6.716 + t^6.942/g1^18 + 2*g1^26*t^6.972 + t^7.085/g1^8 + g1^36*t^7.116 + g1^2*t^7.229 + g1^46*t^7.259 + 2*g1^12*t^7.372 + g1^22*t^7.515 + (2*t^7.628)/g1^12 + 2*g1^32*t^7.658 + t^7.771/g1^2 + 2*g1^42*t^7.801 + g1^8*t^7.915 + t^8.028/g1^26 - g1^18*t^8.058 + (2*t^8.171)/g1^16 + 2*g1^28*t^8.201 + g1^72*t^8.231 - t^8.314/g1^6 + g1^38*t^8.344 + 2*g1^4*t^8.457 + g1^48*t^8.487 + t^8.57/g1^30 - g1^14*t^8.6 + t^8.714/g1^20 + 2*g1^24*t^8.744 + g1^68*t^8.774 - (2*t^8.857)/g1^10 + g1^34*t^8.887 - (g1^2*t^4.229)/y - (g1^20*t^6.286)/y - (g1^16*t^6.829)/y - t^7.085/(g1^8*y) + (2*g1^12*t^7.372)/y + t^7.628/(g1^12*y) + (g1^32*t^7.658)/y + (2*g1^8*t^7.915)/y + (g1^18*t^8.058)/y + (2*t^8.171)/(g1^16*y) + t^8.314/(g1^6*y) - (g1^38*t^8.344)/y + (g1^4*t^8.457)/y + (3*g1^14*t^8.6)/y + (g1^24*t^8.744)/y + (3*t^8.857)/(g1^10*y) - (g1^34*t^8.887)/y - g1^2*t^4.229*y - g1^20*t^6.286*y - g1^16*t^6.829*y - (t^7.085*y)/g1^8 + 2*g1^12*t^7.372*y + (t^7.628*y)/g1^12 + g1^32*t^7.658*y + 2*g1^8*t^7.915*y + g1^18*t^8.058*y + (2*t^8.171*y)/g1^16 + (t^8.314*y)/g1^6 - g1^38*t^8.344*y + g1^4*t^8.457*y + 3*g1^14*t^8.6*y + g1^24*t^8.744*y + (3*t^8.857*y)/g1^10 - g1^34*t^8.887*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
50917 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}^{2}$ 0.5847 0.7249 0.8065 [M:[1.2444, 0.7331, 0.7556, 0.926, 1.1704, 1.0], q:[0.463, 0.2926], qb:[0.8039, 0.7813], phi:[0.4148]] t^2.199 + t^2.267 + t^2.778 + t^3. + t^3.289 + 2*t^3.511 + t^3.733 + t^4.023 + t^4.399 + t^4.466 + t^4.534 + t^4.756 + t^4.977 + t^5.045 + t^5.199 + t^5.267 + 2*t^5.556 + t^5.711 + 2*t^5.778 + t^5.932 - t^6. - t^4.244/y - t^4.244*y detail