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
56250 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}M_{7}$ + ${ }M_{5}\phi_{1}^{2}$ 0.6537 0.8118 0.8053 [M:[1.1758, 1.0604, 0.8242, 0.8224, 1.0586, 0.7051, 1.1776], q:[0.4112, 0.413], qb:[0.5284, 0.7647], phi:[0.4707]] [M:[[12], [-30], [-12], [22], [4], [14], [-22]], q:[[11], [-23]], qb:[[19], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{6}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{2}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{5}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{6}\phi_{1}q_{1}^{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ ${}$ -1 t^2.115 + t^2.472 + t^2.824 + t^3.176 + t^3.181 + t^3.528 + t^3.533 + 2*t^3.879 + t^3.89 + 2*t^4.231 + t^4.236 + t^4.583 + t^4.588 + t^4.94 + t^4.945 + t^5.291 + 2*t^5.297 + t^5.643 + 2*t^5.648 + t^5.995 - t^6. + 2*t^6.005 + t^6.346 + 2*t^6.352 + t^6.357 + 2*t^6.362 + t^6.698 + 3*t^6.703 + t^6.709 + 2*t^6.714 + 3*t^7.055 + 2*t^7.06 + t^7.071 + 3*t^7.407 + 2*t^7.412 + t^7.417 + t^7.423 + 3*t^7.758 + 2*t^7.764 + 2*t^7.769 + t^7.78 + 3*t^8.11 - t^8.115 + 2*t^8.121 + t^8.126 + 3*t^8.462 + t^8.472 + 2*t^8.478 + 2*t^8.813 + 2*t^8.819 - t^8.824 + 2*t^8.83 + t^8.835 - t^4.412/y - t^6.528/y + t^7.231/y + t^7.588/y - t^7.593/y + t^7.94/y + t^8.291/y + (3*t^8.297)/y + (2*t^8.648)/y + t^8.654/y + (2*t^8.995)/y - t^4.412*y - t^6.528*y + t^7.231*y + t^7.588*y - t^7.593*y + t^7.94*y + t^8.291*y + 3*t^8.297*y + 2*t^8.648*y + t^8.654*y + 2*t^8.995*y g1^14*t^2.115 + t^2.472/g1^12 + t^2.824/g1^4 + g1^4*t^3.176 + t^3.181/g1^30 + g1^12*t^3.528 + t^3.533/g1^22 + 2*g1^20*t^3.879 + t^3.89/g1^48 + 2*g1^28*t^4.231 + t^4.236/g1^6 + g1^36*t^4.583 + g1^2*t^4.588 + g1^10*t^4.94 + t^4.945/g1^24 + g1^18*t^5.291 + (2*t^5.297)/g1^16 + g1^26*t^5.643 + (2*t^5.648)/g1^8 + g1^34*t^5.995 - t^6. + (2*t^6.005)/g1^34 + g1^42*t^6.346 + 2*g1^8*t^6.352 + t^6.357/g1^26 + (2*t^6.362)/g1^60 + g1^50*t^6.698 + 3*g1^16*t^6.703 + t^6.709/g1^18 + (2*t^6.714)/g1^52 + 3*g1^24*t^7.055 + (2*t^7.06)/g1^10 + t^7.071/g1^78 + 3*g1^32*t^7.407 + (2*t^7.412)/g1^2 + t^7.417/g1^36 + t^7.423/g1^70 + 3*g1^40*t^7.758 + 2*g1^6*t^7.764 + (2*t^7.769)/g1^28 + t^7.78/g1^96 + 3*g1^48*t^8.11 - g1^14*t^8.115 + (2*t^8.121)/g1^20 + t^8.126/g1^54 + 3*g1^56*t^8.462 + t^8.472/g1^12 + (2*t^8.478)/g1^46 + 2*g1^64*t^8.813 + 2*g1^30*t^8.819 - t^8.824/g1^4 + (2*t^8.83)/g1^38 + t^8.835/g1^72 - t^4.412/(g1^2*y) - (g1^12*t^6.528)/y + (g1^28*t^7.231)/y + (g1^2*t^7.588)/y - t^7.593/(g1^32*y) + (g1^10*t^7.94)/y + (g1^18*t^8.291)/y + (3*t^8.297)/(g1^16*y) + (2*t^8.648)/(g1^8*y) + t^8.654/(g1^42*y) + (2*g1^34*t^8.995)/y - (t^4.412*y)/g1^2 - g1^12*t^6.528*y + g1^28*t^7.231*y + g1^2*t^7.588*y - (t^7.593*y)/g1^32 + g1^10*t^7.94*y + g1^18*t^8.291*y + (3*t^8.297*y)/g1^16 + (2*t^8.648*y)/g1^8 + (t^8.654*y)/g1^42 + 2*g1^34*t^8.995*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
51119 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}M_{7}$ 0.6704 0.8308 0.8069 [M:[1.1573, 0.9835, 0.8427, 0.7473, 0.8881, 0.7246, 1.2527], q:[0.3736, 0.4691], qb:[0.6428, 0.7836], phi:[0.4327]] t^2.174 + t^2.528 + t^2.596 + t^2.664 + t^2.951 + t^3.472 + t^3.54 + t^3.758 + t^4.112 + t^4.279 + 2*t^4.348 + t^4.634 + t^4.702 + t^4.77 + t^4.838 + t^5.056 + 2*t^5.124 + t^5.155 + t^5.192 + t^5.261 + t^5.329 + t^5.547 + t^5.615 + t^5.646 + t^5.901 + t^5.932 - 2*t^6. - t^4.298/y - t^4.298*y detail