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
1393 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{4}M_{6}$ 0.7132 0.878 0.8122 [M:[1.0, 0.8894, 0.834, 1.0553, 1.0, 0.9447], q:[0.583, 0.417], qb:[0.583, 0.5277], phi:[0.4723]] [M:[[0], [-4], [-6], [2], [0], [-2]], q:[[3], [-3]], qb:[[3], [1]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ ${}M_{1}M_{5}$ -2 t^2.502 + t^2.668 + 2*t^2.834 + 2*t^3. + t^3.332 + t^3.919 + t^4.251 + 2*t^4.417 + t^4.583 + 2*t^4.749 + 3*t^4.915 + t^5.004 + t^5.17 + 3*t^5.336 + 2*t^5.502 + 4*t^5.668 + 3*t^5.834 - 2*t^6. + t^6.421 - 2*t^6.498 + t^6.587 + t^6.664 + 3*t^6.753 + 3*t^6.919 + 3*t^7.085 + 6*t^7.251 + 4*t^7.417 + t^7.506 + 4*t^7.583 + t^7.672 + 5*t^7.749 + 4*t^7.838 + t^7.915 + 3*t^8.004 - 2*t^8.081 + 5*t^8.17 + t^8.247 + 5*t^8.336 + 2*t^8.502 + 2*t^8.668 - 4*t^8.834 + t^8.923 - t^4.417/y - t^6.919/y - t^7.085/y - t^7.251/y + t^7.583/y + t^7.749/y + t^7.915/y + t^8.17/y + (2*t^8.336)/y + (4*t^8.502)/y + (3*t^8.668)/y + (5*t^8.834)/y - t^4.417*y - t^6.919*y - t^7.085*y - t^7.251*y + t^7.583*y + t^7.749*y + t^7.915*y + t^8.17*y + 2*t^8.336*y + 4*t^8.502*y + 3*t^8.668*y + 5*t^8.834*y t^2.502/g1^6 + t^2.668/g1^4 + (2*t^2.834)/g1^2 + 2*t^3. + g1^4*t^3.332 + t^3.919/g1^7 + t^4.251/g1^3 + (2*t^4.417)/g1 + g1*t^4.583 + 2*g1^3*t^4.749 + 3*g1^5*t^4.915 + t^5.004/g1^12 + t^5.17/g1^10 + (3*t^5.336)/g1^8 + (2*t^5.502)/g1^6 + (4*t^5.668)/g1^4 + (3*t^5.834)/g1^2 - 2*t^6. + t^6.421/g1^13 - 2*g1^6*t^6.498 + t^6.587/g1^11 + g1^8*t^6.664 + (3*t^6.753)/g1^9 + (3*t^6.919)/g1^7 + (3*t^7.085)/g1^5 + (6*t^7.251)/g1^3 + (4*t^7.417)/g1 + t^7.506/g1^18 + 4*g1*t^7.583 + t^7.672/g1^16 + 5*g1^3*t^7.749 + (4*t^7.838)/g1^14 + g1^5*t^7.915 + (3*t^8.004)/g1^12 - 2*g1^7*t^8.081 + (5*t^8.17)/g1^10 + g1^9*t^8.247 + (5*t^8.336)/g1^8 + (2*t^8.502)/g1^6 + (2*t^8.668)/g1^4 - (4*t^8.834)/g1^2 + t^8.923/g1^19 - t^4.417/(g1*y) - t^6.919/(g1^7*y) - t^7.085/(g1^5*y) - t^7.251/(g1^3*y) + (g1*t^7.583)/y + (g1^3*t^7.749)/y + (g1^5*t^7.915)/y + t^8.17/(g1^10*y) + (2*t^8.336)/(g1^8*y) + (4*t^8.502)/(g1^6*y) + (3*t^8.668)/(g1^4*y) + (5*t^8.834)/(g1^2*y) - (t^4.417*y)/g1 - (t^6.919*y)/g1^7 - (t^7.085*y)/g1^5 - (t^7.251*y)/g1^3 + g1*t^7.583*y + g1^3*t^7.749*y + g1^5*t^7.915*y + (t^8.17*y)/g1^10 + (2*t^8.336*y)/g1^8 + (4*t^8.502*y)/g1^6 + (3*t^8.668*y)/g1^4 + (5*t^8.834*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
2454 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{4}M_{6}$ + ${ }M_{3}M_{7}$ 0.7007 0.8557 0.8188 [M:[1.0, 0.9231, 0.8846, 1.0385, 1.0, 0.9615, 1.1154], q:[0.5577, 0.4423], qb:[0.5577, 0.5192], phi:[0.4808]] t^2.769 + 2*t^2.885 + 2*t^3. + t^3.231 + t^3.346 + t^4.096 + t^4.327 + 2*t^4.442 + t^4.558 + 2*t^4.673 + 3*t^4.789 + t^5.538 + 4*t^5.769 + 2*t^5.885 - 2*t^6. - t^4.442/y - t^4.442*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
912 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}\phi_{1}^{2}$ 0.7083 0.8692 0.8149 [M:[1.0, 0.9016, 0.8525, 1.0492, 1.0], q:[0.5738, 0.4262], qb:[0.5738, 0.5246], phi:[0.4754]] t^2.557 + t^2.705 + t^2.852 + 2*t^3. + t^3.148 + t^3.295 + t^3.984 + t^4.279 + 2*t^4.426 + t^4.574 + 2*t^4.721 + 3*t^4.869 + t^5.115 + t^5.262 + 2*t^5.41 + t^5.557 + 3*t^5.705 + 2*t^5.852 - t^6. - t^4.426/y - t^4.426*y detail