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
1492 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{5}M_{6}$ 0.6999 0.8585 0.8152 [M:[0.9245, 1.0252, 1.0, 0.9496, 1.0504, 0.9496], q:[0.563, 0.5126], qb:[0.437, 0.5378], phi:[0.4874]] [M:[[-6], [2], [0], [-4], [4], [-4]], q:[[5], [1]], qb:[[-5], [3]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }M_{4}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{3}\phi_{1}^{2}$ ${}$ -2 t^2.773 + 2*t^2.849 + t^2.924 + t^3. + t^3.076 + t^3.302 + t^4.085 + t^4.311 + t^4.387 + t^4.462 + t^4.538 + t^4.613 + 2*t^4.689 + t^4.764 + t^4.84 + t^5.547 + t^5.622 + 3*t^5.698 + 2*t^5.773 + 3*t^5.849 + t^5.924 - 2*t^6. + t^6.151 + t^6.604 + t^6.858 + 2*t^6.933 + t^7.009 + t^7.085 + 2*t^7.16 + 2*t^7.236 + 3*t^7.311 + 3*t^7.387 + 2*t^7.462 + 3*t^7.538 + 3*t^7.613 + 3*t^7.689 + t^7.764 + t^7.991 + t^8.067 + t^8.142 + t^8.169 + t^8.32 + 2*t^8.396 + 2*t^8.471 + 4*t^8.547 + 4*t^8.622 + 3*t^8.698 + 2*t^8.773 - 3*t^8.849 - 2*t^8.924 - t^4.462/y - t^7.236/y - t^7.311/y + t^7.613/y + t^7.689/y + (2*t^8.622)/y + (2*t^8.698)/y + (3*t^8.773)/y + (3*t^8.849)/y + (3*t^8.924)/y - t^4.462*y - t^7.236*y - t^7.311*y + t^7.613*y + t^7.689*y + 2*t^8.622*y + 2*t^8.698*y + 3*t^8.773*y + 3*t^8.849*y + 3*t^8.924*y t^2.773/g1^6 + (2*t^2.849)/g1^4 + t^2.924/g1^2 + t^3. + g1^2*t^3.076 + g1^8*t^3.302 + t^4.085/g1^11 + t^4.311/g1^5 + t^4.387/g1^3 + t^4.462/g1 + g1*t^4.538 + g1^3*t^4.613 + 2*g1^5*t^4.689 + g1^7*t^4.764 + g1^9*t^4.84 + t^5.547/g1^12 + t^5.622/g1^10 + (3*t^5.698)/g1^8 + (2*t^5.773)/g1^6 + (3*t^5.849)/g1^4 + t^5.924/g1^2 - 2*t^6. + g1^4*t^6.151 + g1^16*t^6.604 + t^6.858/g1^17 + (2*t^6.933)/g1^15 + t^7.009/g1^13 + t^7.085/g1^11 + (2*t^7.16)/g1^9 + (2*t^7.236)/g1^7 + (3*t^7.311)/g1^5 + (3*t^7.387)/g1^3 + (2*t^7.462)/g1 + 3*g1*t^7.538 + 3*g1^3*t^7.613 + 3*g1^5*t^7.689 + g1^7*t^7.764 + g1^13*t^7.991 + g1^15*t^8.067 + g1^17*t^8.142 + t^8.169/g1^22 + t^8.32/g1^18 + (2*t^8.396)/g1^16 + (2*t^8.471)/g1^14 + (4*t^8.547)/g1^12 + (4*t^8.622)/g1^10 + (3*t^8.698)/g1^8 + (2*t^8.773)/g1^6 - (3*t^8.849)/g1^4 - (2*t^8.924)/g1^2 - t^4.462/(g1*y) - t^7.236/(g1^7*y) - t^7.311/(g1^5*y) + (g1^3*t^7.613)/y + (g1^5*t^7.689)/y + (2*t^8.622)/(g1^10*y) + (2*t^8.698)/(g1^8*y) + (3*t^8.773)/(g1^6*y) + (3*t^8.849)/(g1^4*y) + (3*t^8.924)/(g1^2*y) - (t^4.462*y)/g1 - (t^7.236*y)/g1^7 - (t^7.311*y)/g1^5 + g1^3*t^7.613*y + g1^5*t^7.689*y + (2*t^8.622*y)/g1^10 + (2*t^8.698*y)/g1^8 + (3*t^8.773*y)/g1^6 + (3*t^8.849*y)/g1^4 + (3*t^8.924*y)/g1^2


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
2584 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{2}M_{7}$ 0.7024 0.8631 0.8138 [M:[0.9142, 1.0286, 1.0, 0.9428, 1.0572, 0.9428, 0.9714], q:[0.5715, 0.5143], qb:[0.4285, 0.5429], phi:[0.4857]] t^2.743 + 2*t^2.828 + 2*t^2.914 + t^3. + t^3.343 + t^4.028 + t^4.285 + t^4.371 + t^4.457 + t^4.543 + t^4.629 + 2*t^4.715 + t^4.8 + t^4.886 + t^5.485 + t^5.571 + 4*t^5.657 + 4*t^5.743 + 4*t^5.828 - 3*t^6. - t^4.457/y - t^4.457*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
960 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}^{2}$ 0.6958 0.8515 0.8172 [M:[0.9451, 1.0183, 1.0, 0.9634, 1.0366], q:[0.5458, 0.5092], qb:[0.4542, 0.5275], phi:[0.4908]] t^2.835 + t^2.89 + t^2.945 + t^3. + t^3.055 + t^3.11 + t^3.22 + t^4.198 + t^4.363 + t^4.418 + t^4.473 + t^4.527 + t^4.582 + 2*t^4.637 + t^4.692 + t^4.747 + t^5.67 + t^5.78 + t^5.835 + 2*t^5.89 + t^5.945 - t^6. - t^4.473/y - t^4.473*y detail