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
1925 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}^{4}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ 0.666 0.8535 0.7803 [M:[0.8191, 1.1809, 0.8191, 0.7236, 1.1382, 0.8191], q:[0.75, 0.4309], qb:[0.3882, 0.4309], phi:[0.5]] [M:[[1, 1], [-1, -1], [1, 1], [-2, 0], [1, 0], [0, -1]], q:[[0, 0], [-1, -1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{6}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }M_{5}M_{6}$, ${ }M_{6}q_{1}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{3}q_{1}\tilde{q}_{1}$ ${}$ -5 t^2.171 + 4*t^2.457 + t^3. + 2*t^3.415 + 2*t^3.957 + 3*t^4.085 + t^4.342 + 4*t^4.628 + 10*t^4.915 + t^5.171 + 4*t^5.457 + 2*t^5.585 + 6*t^5.872 - 5*t^6. + 3*t^6.256 + 8*t^6.415 + t^6.513 + 8*t^6.543 + 4*t^6.799 + 2*t^6.829 - 2*t^6.957 + 9*t^7.085 + t^7.342 + 20*t^7.372 - 2*t^7.5 + 2*t^7.756 + 9*t^7.915 + 8*t^8.043 + 12*t^8.329 + 3*t^8.427 - 20*t^8.457 + t^8.684 + 8*t^8.714 + 18*t^8.872 + 4*t^8.97 - t^4.5/y - t^6.671/y - (2*t^6.957)/y + t^7.085/y + (4*t^7.628)/y + (5*t^7.915)/y + (2*t^8.043)/y + t^8.171/y + t^8.329/y + (4*t^8.457)/y + (2*t^8.585)/y - t^8.842/y + (8*t^8.872)/y - t^4.5*y - t^6.671*y - 2*t^6.957*y + t^7.085*y + 4*t^7.628*y + 5*t^7.915*y + 2*t^8.043*y + t^8.171*y + t^8.329*y + 4*t^8.457*y + 2*t^8.585*y - t^8.842*y + 8*t^8.872*y t^2.171/g1^2 + (2*t^2.457)/g2 + 2*g1*g2*t^2.457 + t^3. + 2*g1*t^3.415 + t^3.957/g2 + g1*g2*t^3.957 + t^4.085/g1 + t^4.085/(g1^2*g2^2) + g2^2*t^4.085 + t^4.342/g1^4 + (2*t^4.628)/(g1^2*g2) + (2*g2*t^4.628)/g1 + 4*g1*t^4.915 + (3*t^4.915)/g2^2 + 3*g1^2*g2^2*t^4.915 + t^5.171/g1^2 + (2*t^5.457)/g2 + 2*g1*g2*t^5.457 + (2*t^5.585)/g1 + (3*g1*t^5.872)/g2 + 3*g1^2*g2*t^5.872 - 3*t^6. - t^6./(g1*g2^2) - g1*g2^2*t^6. + t^6.256/g1^3 + t^6.256/(g1^4*g2^2) + (g2^2*t^6.256)/g1^2 + 4*g1*t^6.415 + (2*t^6.415)/g2^2 + 2*g1^2*g2^2*t^6.415 + t^6.513/g1^6 + (2*t^6.543)/(g1^2*g2^3) + (2*t^6.543)/(g1*g2) + 2*g2*t^6.543 + 2*g1*g2^3*t^6.543 + (2*t^6.799)/(g1^4*g2) + (2*g2*t^6.799)/g1^3 + 2*g1^2*t^6.829 - t^6.957/g2 - g1*g2*t^6.957 + (3*t^7.085)/g1 + (3*t^7.085)/(g1^2*g2^2) + 3*g2^2*t^7.085 + t^7.342/g1^4 + (4*t^7.372)/g2^3 + (6*g1*t^7.372)/g2 + 6*g1^2*g2*t^7.372 + 4*g1^3*g2^3*t^7.372 - 2*t^7.5 + (2*t^7.756)/g1^3 + 3*g1*t^7.915 + (3*t^7.915)/g2^2 + 3*g1^2*g2^2*t^7.915 + t^8.043/(g1^2*g2^3) + (3*t^8.043)/(g1*g2) + 3*g2*t^8.043 + g1*g2^3*t^8.043 - (2*t^8.171)/g1^2 + t^8.171/(g1^4*g2^4) + g2^4*t^8.171 + 4*g1^2*t^8.329 + (4*g1*t^8.329)/g2^2 + 4*g1^3*g2^2*t^8.329 + t^8.427/g1^5 + t^8.427/(g1^6*g2^2) + (g2^2*t^8.427)/g1^4 - (2*t^8.457)/(g1*g2^3) - (8*t^8.457)/g2 - 8*g1*g2*t^8.457 - 2*g1^2*g2^3*t^8.457 + t^8.684/g1^8 + (2*t^8.714)/(g1^4*g2^3) + (2*t^8.714)/(g1^3*g2) + (2*g2*t^8.714)/g1^2 + (2*g2^3*t^8.714)/g1 + (3*t^8.872)/g2^3 + (6*g1*t^8.872)/g2 + 6*g1^2*g2*t^8.872 + 3*g1^3*g2^3*t^8.872 + (2*t^8.97)/(g1^6*g2) + (2*g2*t^8.97)/g1^5 - t^4.5/y - t^6.671/(g1^2*y) - t^6.957/(g2*y) - (g1*g2*t^6.957)/y + t^7.085/(g1*y) + (2*t^7.628)/(g1^2*g2*y) + (2*g2*t^7.628)/(g1*y) + (3*g1*t^7.915)/y + t^7.915/(g2^2*y) + (g1^2*g2^2*t^7.915)/y + t^8.043/(g1*g2*y) + (g2*t^8.043)/y + t^8.171/(g1^2*y) + (g1^2*t^8.329)/y + (2*t^8.457)/(g2*y) + (2*g1*g2*t^8.457)/y + (2*t^8.585)/(g1*y) - t^8.842/(g1^4*y) + (4*g1*t^8.872)/(g2*y) + (4*g1^2*g2*t^8.872)/y - t^4.5*y - (t^6.671*y)/g1^2 - (t^6.957*y)/g2 - g1*g2*t^6.957*y + (t^7.085*y)/g1 + (2*t^7.628*y)/(g1^2*g2) + (2*g2*t^7.628*y)/g1 + 3*g1*t^7.915*y + (t^7.915*y)/g2^2 + g1^2*g2^2*t^7.915*y + (t^8.043*y)/(g1*g2) + g2*t^8.043*y + (t^8.171*y)/g1^2 + g1^2*t^8.329*y + (2*t^8.457*y)/g2 + 2*g1*g2*t^8.457*y + (2*t^8.585*y)/g1 - (t^8.842*y)/g1^4 + (4*g1*t^8.872*y)/g2 + 4*g1^2*g2*t^8.872*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
567 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}^{4}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ 0.6514 0.8288 0.7859 [M:[0.8067, 1.1933, 0.8067, 0.7089, 1.1456], q:[0.75, 0.4433], qb:[0.3956, 0.4111], phi:[0.5]] t^2.127 + 2*t^2.42 + t^2.517 + t^3. + 2*t^3.437 + t^3.483 + t^3.92 + t^3.967 + t^4.017 + t^4.063 + t^4.16 + t^4.253 + 2*t^4.547 + t^4.643 + 3*t^4.84 + 2*t^4.937 + t^5.033 + t^5.127 + 2*t^5.42 + t^5.517 + 2*t^5.563 + t^5.61 + 3*t^5.857 + t^5.903 + t^5.953 - 2*t^6. - t^4.5/y - t^4.5*y detail