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
564 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ 0.6272 0.8162 0.7685 [M:[0.9767, 1.0698, 0.7442, 0.7442], q:[0.7442, 0.2791], qb:[0.4651, 0.4651], phi:[0.5116]] [M:[[4], [-12], [1], [1]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ ${}$ -5 4*t^2.233 + t^2.93 + t^3.07 + 2*t^3.209 + 2*t^3.628 + 3*t^4.325 + 10*t^4.465 + 4*t^5.163 + 4*t^5.302 + 6*t^5.442 + 8*t^5.86 - 5*t^6. + t^6.14 + 2*t^6.279 + 3*t^6.419 + 10*t^6.558 + 18*t^6.698 - 2*t^6.977 + 3*t^7.256 + 8*t^7.395 + 8*t^7.535 + 12*t^7.675 + 4*t^7.953 + 14*t^8.093 - 20*t^8.233 + 2*t^8.372 + 6*t^8.512 + 13*t^8.651 + 22*t^8.791 + 22*t^8.93 - t^4.535/y - (2*t^6.767)/y + t^7.325/y + (6*t^7.465)/y - t^7.744/y + (4*t^8.163)/y + (6*t^8.302)/y + (8*t^8.442)/y + (8*t^8.86)/y - t^4.535*y - 2*t^6.767*y + t^7.325*y + 6*t^7.465*y - t^7.744*y + 4*t^8.163*y + 6*t^8.302*y + 8*t^8.442*y + 8*t^8.86*y 4*g1*t^2.233 + g1^4*t^2.93 + t^3.07/g1^4 + (2*t^3.209)/g1^12 + 2*g1^7*t^3.628 + 3*g1^10*t^4.325 + 10*g1^2*t^4.465 + 4*g1^5*t^5.163 + (4*t^5.302)/g1^3 + (6*t^5.442)/g1^11 + 8*g1^8*t^5.86 - 5*t^6. + t^6.14/g1^8 + (2*t^6.279)/g1^16 + (3*t^6.419)/g1^24 + 10*g1^11*t^6.558 + 18*g1^3*t^6.698 - (2*t^6.977)/g1^13 + 3*g1^14*t^7.256 + 8*g1^6*t^7.395 + (8*t^7.535)/g1^2 + (12*t^7.675)/g1^10 + 4*g1^17*t^7.953 + 14*g1^9*t^8.093 - 20*g1*t^8.233 + (2*t^8.372)/g1^7 + (6*t^8.512)/g1^15 + (8*t^8.651)/g1^23 + 5*g1^20*t^8.651 + 22*g1^12*t^8.791 + 22*g1^4*t^8.93 - t^4.535/(g1^2*y) - (2*t^6.767)/(g1*y) + (g1^10*t^7.325)/y + (6*g1^2*t^7.465)/y - t^7.744/(g1^14*y) + (4*g1^5*t^8.163)/y + (6*t^8.302)/(g1^3*y) + (8*t^8.442)/(g1^11*y) + (8*g1^8*t^8.86)/y - (t^4.535*y)/g1^2 - (2*t^6.767*y)/g1 + g1^10*t^7.325*y + 6*g1^2*t^7.465*y - (t^7.744*y)/g1^14 + 4*g1^5*t^8.163*y + (6*t^8.302*y)/g1^3 + (8*t^8.442*y)/g1^11 + 8*g1^8*t^8.86*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
1908 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ 0.6447 0.8471 0.7611 [M:[0.9845, 1.0466, 0.7461, 0.7461, 0.7772], q:[0.7461, 0.2694], qb:[0.4767, 0.4767], phi:[0.5078]] 4*t^2.238 + t^2.332 + t^2.953 + t^3.047 + 2*t^3.14 + t^3.668 + 3*t^4.383 + 10*t^4.477 + 4*t^4.57 + t^4.663 + 4*t^5.192 + 5*t^5.285 + 7*t^5.378 + 2*t^5.471 + 4*t^5.907 - 4*t^6. - t^4.523/y - t^4.523*y detail


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
355 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ 0.608 0.7809 0.7786 [M:[0.9776, 1.0673, 0.7444], q:[0.7444, 0.2781], qb:[0.4663, 0.4663], phi:[0.5112]] 3*t^2.233 + t^2.933 + t^3.067 + 2*t^3.202 + 2*t^3.632 + t^3.767 + 3*t^4.332 + 6*t^4.466 + 3*t^5.166 + 3*t^5.3 + 4*t^5.435 + 6*t^5.865 - 2*t^6. - t^4.534/y - t^4.534*y detail