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
61253 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{6}$ 1.3971 1.5951 0.8759 [X:[1.3333], M:[0.8333], q:[0.6667, 0.3333], qb:[0.5, 0.5], phi:[0.3333]] [X:[[0]], M:[[0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 1073/768, c: 1225/768, X1: 4/3, M1: 5/6, q1: 2/3, q2: 1/3, qb1: 1/2, qb2: 1/2, phi1: 1/3}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ 6 3*t^2.5 + t^3. + 3*t^3.5 + t^4. + 4*t^4.5 + 6*t^5. + 7*t^5.5 + 6*t^6. + 8*t^6.5 + 13*t^7. + 15*t^7.5 + 21*t^8. + 9*t^8.5 - t^4./y - t^5./y - (3*t^6.5)/y - t^7./y - (4*t^7.5)/y + (2*t^8.)/y - t^4.*y - t^5.*y - 3*t^6.5*y - t^7.*y - 4*t^7.5*y + 2*t^8.*y 3*t^2.5 + t^3. + 3*t^3.5 + t^4. + 4*t^4.5 + 6*t^5. + 7*t^5.5 + 6*t^6. + 8*t^6.5 + 13*t^7. + 15*t^7.5 + 21*t^8. + 9*t^8.5 - t^4./y - t^5./y - (3*t^6.5)/y - t^7./y - (4*t^7.5)/y + (2*t^8.)/y - t^4.*y - t^5.*y - 3*t^6.5*y - t^7.*y - 4*t^7.5*y + 2*t^8.*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
60095 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ 1.4 1.5947 0.8779 [X:[1.3491], M:[0.79], q:[0.6667, 0.3412], qb:[0.4961, 0.5434], phi:[0.3254]] t^2.37 + t^2.51 + t^2.65 + t^2.93 + 2*t^3.49 + t^3.63 + t^4.05 + 2*t^4.46 + 2*t^4.61 + t^4.74 + t^4.88 + 2*t^5.02 + t^5.17 + t^5.3 + t^5.31 + 2*t^5.44 + 3*t^5.58 + t^5.72 + 2*t^5.86 + t^6. - t^3.98/y - t^4.95/y - t^3.98*y - t^4.95*y detail