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
46274 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ 0.6895 0.8745 0.7884 [M:[0.6951, 0.6921, 0.6981, 0.6921], q:[0.8262, 0.8262], qb:[0.4817, 0.4756], phi:[0.3476]] [M:[[-4, -4], [-7, -1], [-1, -7], [-7, -1]], q:[[1, 1], [1, 1]], qb:[[6, 0], [0, 6]], phi:[[-2, -2]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{4}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ ${}$ -2 2*t^2.076 + 2*t^2.085 + t^2.094 + t^2.872 + t^3.897 + t^3.906 + t^3.933 + 3*t^4.152 + 4*t^4.162 + 5*t^4.171 + 2*t^4.18 + t^4.189 + 2*t^4.948 + 3*t^4.957 + t^4.966 + t^5.744 + 2*t^5.973 + 3*t^5.982 + t^5.991 - 2*t^6. + t^6.018 + t^6.027 + 4*t^6.229 + 6*t^6.238 + 9*t^6.247 + 8*t^6.256 + 5*t^6.265 + 2*t^6.274 + t^6.283 + t^6.769 + t^6.778 + t^6.805 + 2*t^7.025 + 4*t^7.034 + 5*t^7.043 + t^7.052 + t^7.793 + t^7.802 + t^7.829 - t^7.848 + t^7.866 + 3*t^8.049 + 5*t^8.058 + 3*t^8.067 - 4*t^8.076 - 5*t^8.085 - 4*t^8.094 + t^8.103 + t^8.113 + t^8.122 + 5*t^8.305 + 8*t^8.314 + 13*t^8.323 + 14*t^8.332 + 14*t^8.341 + 8*t^8.35 + 5*t^8.359 + 2*t^8.368 + t^8.378 + t^8.616 + 2*t^8.845 + 3*t^8.854 - 4*t^8.872 - 2*t^8.881 + t^8.89 + t^8.899 - t^4.043/y - (2*t^6.119)/y - (2*t^6.128)/y - t^6.137/y + t^7.152/y + (4*t^7.162)/y + (3*t^7.171)/y + (2*t^7.18)/y + (3*t^7.948)/y + (4*t^7.957)/y + (3*t^7.966)/y - (3*t^8.195)/y - (4*t^8.204)/y - (5*t^8.213)/y - (2*t^8.222)/y - t^8.231/y + (2*t^8.973)/y + (4*t^8.982)/y + (3*t^8.991)/y - t^4.043*y - 2*t^6.119*y - 2*t^6.128*y - t^6.137*y + t^7.152*y + 4*t^7.162*y + 3*t^7.171*y + 2*t^7.18*y + 3*t^7.948*y + 4*t^7.957*y + 3*t^7.966*y - 3*t^8.195*y - 4*t^8.204*y - 5*t^8.213*y - 2*t^8.222*y - t^8.231*y + 2*t^8.973*y + 4*t^8.982*y + 3*t^8.991*y (2*t^2.076)/(g1^7*g2) + (2*t^2.085)/(g1^4*g2^4) + t^2.094/(g1*g2^7) + g1^6*g2^6*t^2.872 + (g2^10*t^3.897)/g1^2 + g1*g2^7*t^3.906 + (g1^10*t^3.933)/g2^2 + (3*t^4.152)/(g1^14*g2^2) + (4*t^4.162)/(g1^11*g2^5) + (5*t^4.171)/(g1^8*g2^8) + (2*t^4.18)/(g1^5*g2^11) + t^4.189/(g1^2*g2^14) + (2*g2^5*t^4.948)/g1 + 3*g1^2*g2^2*t^4.957 + (g1^5*t^4.966)/g2 + g1^12*g2^12*t^5.744 + (2*g2^9*t^5.973)/g1^9 + (3*g2^6*t^5.982)/g1^6 + (g2^3*t^5.991)/g1^3 - 2*t^6. + (g1^6*t^6.018)/g2^6 + (g1^9*t^6.027)/g2^9 + (4*t^6.229)/(g1^21*g2^3) + (6*t^6.238)/(g1^18*g2^6) + (9*t^6.247)/(g1^15*g2^9) + (8*t^6.256)/(g1^12*g2^12) + (5*t^6.265)/(g1^9*g2^15) + (2*t^6.274)/(g1^6*g2^18) + t^6.283/(g1^3*g2^21) + g1^4*g2^16*t^6.769 + g1^7*g2^13*t^6.778 + g1^16*g2^4*t^6.805 + (2*g2^4*t^7.025)/g1^8 + (4*g2*t^7.034)/g1^5 + (5*t^7.043)/(g1^2*g2^2) + (g1*t^7.052)/g2^5 + (g2^20*t^7.793)/g1^4 + (g2^17*t^7.802)/g1 + g1^8*g2^8*t^7.829 - g1^14*g2^2*t^7.848 + (g1^20*t^7.866)/g2^4 + (3*g2^8*t^8.049)/g1^16 + (5*g2^5*t^8.058)/g1^13 + (3*g2^2*t^8.067)/g1^10 - (4*t^8.076)/(g1^7*g2) - (5*t^8.085)/(g1^4*g2^4) - (4*t^8.094)/(g1*g2^7) + (g1^2*t^8.103)/g2^10 + (g1^5*t^8.113)/g2^13 + (g1^8*t^8.122)/g2^16 + (5*t^8.305)/(g1^28*g2^4) + (8*t^8.314)/(g1^25*g2^7) + (13*t^8.323)/(g1^22*g2^10) + (14*t^8.332)/(g1^19*g2^13) + (14*t^8.341)/(g1^16*g2^16) + (8*t^8.35)/(g1^13*g2^19) + (5*t^8.359)/(g1^10*g2^22) + (2*t^8.368)/(g1^7*g2^25) + t^8.378/(g1^4*g2^28) + g1^18*g2^18*t^8.616 + (2*g2^15*t^8.845)/g1^3 + 3*g2^12*t^8.854 - 4*g1^6*g2^6*t^8.872 - 2*g1^9*g2^3*t^8.881 + g1^12*t^8.89 + (g1^15*t^8.899)/g2^3 - t^4.043/(g1^2*g2^2*y) - (2*t^6.119)/(g1^9*g2^3*y) - (2*t^6.128)/(g1^6*g2^6*y) - t^6.137/(g1^3*g2^9*y) + t^7.152/(g1^14*g2^2*y) + (4*t^7.162)/(g1^11*g2^5*y) + (3*t^7.171)/(g1^8*g2^8*y) + (2*t^7.18)/(g1^5*g2^11*y) + (3*g2^5*t^7.948)/(g1*y) + (4*g1^2*g2^2*t^7.957)/y + (3*g1^5*t^7.966)/(g2*y) - (3*t^8.195)/(g1^16*g2^4*y) - (4*t^8.204)/(g1^13*g2^7*y) - (5*t^8.213)/(g1^10*g2^10*y) - (2*t^8.222)/(g1^7*g2^13*y) - t^8.231/(g1^4*g2^16*y) + (2*g2^9*t^8.973)/(g1^9*y) + (4*g2^6*t^8.982)/(g1^6*y) + (3*g2^3*t^8.991)/(g1^3*y) - (t^4.043*y)/(g1^2*g2^2) - (2*t^6.119*y)/(g1^9*g2^3) - (2*t^6.128*y)/(g1^6*g2^6) - (t^6.137*y)/(g1^3*g2^9) + (t^7.152*y)/(g1^14*g2^2) + (4*t^7.162*y)/(g1^11*g2^5) + (3*t^7.171*y)/(g1^8*g2^8) + (2*t^7.18*y)/(g1^5*g2^11) + (3*g2^5*t^7.948*y)/g1 + 4*g1^2*g2^2*t^7.957*y + (3*g1^5*t^7.966*y)/g2 - (3*t^8.195*y)/(g1^16*g2^4) - (4*t^8.204*y)/(g1^13*g2^7) - (5*t^8.213*y)/(g1^10*g2^10) - (2*t^8.222*y)/(g1^7*g2^13) - (t^8.231*y)/(g1^4*g2^16) + (2*g2^9*t^8.973*y)/g1^9 + (4*g2^6*t^8.982*y)/g1^6 + (3*g2^3*t^8.991*y)/g1^3


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
45978 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ 0.6895 0.8749 0.7881 [M:[0.6959, 0.6857, 0.6931, 0.6986], q:[0.8196, 0.8325], qb:[0.4818, 0.4744], phi:[0.3479]] t^2.057 + t^2.079 + 2*t^2.088 + t^2.096 + t^2.869 + t^3.882 + t^3.89 + t^3.935 + t^4.114 + t^4.136 + 2*t^4.145 + t^4.153 + t^4.159 + 2*t^4.167 + 4*t^4.175 + 2*t^4.183 + t^4.191 + t^4.926 + t^4.948 + 3*t^4.956 + t^4.964 + t^5.737 + t^5.939 + t^5.947 + t^5.961 + 2*t^5.969 + 2*t^5.978 + t^5.986 - 3*t^6. - t^4.044/y - t^4.044*y detail