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
58342 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }q_{2}\tilde{q}_{1}X_{1}$ + ${ }q_{1}\tilde{q}_{1}X_{2}$ + ${ }M_{2}\phi_{1}^{3}$ 1.2686 1.4823 0.8558 [X:[1.4191, 1.3809], M:[0.9809, 0.8], q:[0.4026, 0.3644], qb:[0.2165, 0.6165], phi:[0.4]] [X:[[0, -1], [0, 1]], M:[[0, 1], [0, 0]], q:[[-1, -1], [-1, 1]], qb:[[1, 0], [1, 0]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$ ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ -2 2*t^2.4 + 3*t^2.94 + t^3.06 + 3*t^4.14 + 3*t^4.26 + t^4.35 + t^4.59 + t^4.71 + 2*t^4.8 + 7*t^5.34 + 3*t^5.46 + 3*t^5.55 + t^5.79 + 5*t^5.89 + t^5.91 - 2*t^6. - t^6.45 + 5*t^6.54 + 5*t^6.66 + 4*t^6.75 + t^6.88 + 3*t^6.99 + 8*t^7.09 + 3*t^7.11 + 8*t^7.2 + t^7.22 + t^7.29 + 2*t^7.31 - t^7.41 + 2*t^7.54 + 6*t^7.74 + 2*t^7.86 + 5*t^7.95 + t^8.19 + 18*t^8.29 + t^8.31 + 5*t^8.4 + 7*t^8.49 + 6*t^8.51 + t^8.61 + t^8.7 + 3*t^8.74 + 7*t^8.83 + t^8.85 - 7*t^8.94 + t^8.97 - t^4.2/y - t^5.4/y - (2*t^6.6)/y - (2*t^7.14)/y + (2*t^8.34)/y + (3*t^8.89)/y - t^4.2*y - t^5.4*y - 2*t^6.6*y - 2*t^7.14*y + 2*t^8.34*y + 3*t^8.89*y 2*t^2.4 + 3*g2*t^2.94 + t^3.06/g2 + 3*g2*t^4.14 + (3*t^4.26)/g2 + g1^3*t^4.35 + (g2*t^4.59)/g1^3 + t^4.71/(g1^3*g2) + 2*t^4.8 + 7*g2*t^5.34 + (3*t^5.46)/g2 + 3*g1^3*t^5.55 + (g2*t^5.79)/g1^3 + 5*g2^2*t^5.89 + t^5.91/(g1^3*g2) - 2*t^6. - t^6.45/g1^3 + 5*g2*t^6.54 + (5*t^6.66)/g2 + 4*g1^3*t^6.75 + (g2^3*t^6.88)/g1^3 + (3*g2*t^6.99)/g1^3 + 8*g2^2*t^7.09 + (3*t^7.11)/(g1^3*g2) + 8*t^7.2 + t^7.22/(g1^3*g2^3) + g1^3*g2*t^7.29 + (2*t^7.31)/g2^2 - (g1^3*t^7.41)/g2 + (2*g2^2*t^7.54)/g1^3 + 6*g2*t^7.74 + (2*t^7.86)/g2 + 5*g1^3*t^7.95 + (g2*t^8.19)/g1^3 + 18*g2^2*t^8.29 + t^8.31/(g1^3*g2) + 5*t^8.4 + 7*g1^3*g2*t^8.49 + (6*t^8.51)/g2^2 + (g1^3*t^8.61)/g2 + g1^6*t^8.7 + (3*g2^2*t^8.74)/g1^3 + 7*g2^3*t^8.83 + t^8.85/g1^3 - 7*g2*t^8.94 + t^8.97/(g1^3*g2^2) - t^4.2/y - t^5.4/y - (2*t^6.6)/y - (2*g2*t^7.14)/y + (2*g2*t^8.34)/y + (3*g2^2*t^8.89)/y - t^4.2*y - t^5.4*y - 2*t^6.6*y - 2*g2*t^7.14*y + 2*g2*t^8.34*y + 3*g2^2*t^8.89*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
57342 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }q_{2}\tilde{q}_{1}X_{1}$ + ${ }q_{1}\tilde{q}_{1}X_{2}$ 1.2521 1.4533 0.8616 [X:[1.4191, 1.3809], M:[0.9809], q:[0.4026, 0.3644], qb:[0.2165, 0.6165], phi:[0.4]] t^2.4 + 3*t^2.943 + t^3.057 + t^3.6 + 3*t^4.143 + 3*t^4.257 + t^4.349 + t^4.594 + t^4.709 + 4*t^5.343 + 2*t^5.457 + 3*t^5.549 + t^5.794 + 5*t^5.885 + t^5.909 - t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail