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
61155 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ 1.3737 1.5716 0.8741 [X:[1.3333], M:[0.8333], q:[0.2778, 0.6111], qb:[0.5556, 0.5556], phi:[0.3333]] [X:[[0]], M:[[0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 1055/768, c: 1207/768, X1: 4/3, M1: 5/6, q1: 5/18, q2: 11/18, qb1: 5/9, qb2: 5/9, phi1: 1/3}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$ ${}\phi_{1}^{6}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ 5 3*t^2.5 + t^3. + 3*t^3.5 + t^4. + 5*t^4.5 + 5*t^5. + 8*t^5.5 + 5*t^6. + 8*t^6.5 + 13*t^7. + 13*t^7.5 + 28*t^8. + 5*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. + 5*t^4.5 + 5*t^5. + 8*t^5.5 + 5*t^6. + 8*t^6.5 + 13*t^7. + 13*t^7.5 + 28*t^8. + 5*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
58578 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ 1.4131 1.6407 0.8613 [X:[], M:[0.8804], q:[0.2935, 0.5326], qb:[0.5869, 0.474], phi:[0.3522]] t^2.11 + t^2.3 + 2*t^2.64 + t^3.02 + t^3.17 + t^3.36 + t^3.7 + t^4.08 + t^4.23 + 4*t^4.42 + t^4.6 + 3*t^4.75 + 2*t^4.94 + 3*t^5.13 + 3*t^5.28 + t^5.32 + 4*t^5.47 + 3*t^5.66 + 4*t^5.81 - t^4.06/y - t^5.11/y - t^4.06*y - t^5.11*y detail