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
61177 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{3}\phi_{1}^{3}$ 1.4286 1.6955 0.8426 [X:[], M:[0.7648, 1.1648, 0.8], q:[0.4213, 0.3894], qb:[0.4139, 0.3754], phi:[0.4]] [X:[], M:[[1, 2], [1, 2], [0, 0]], q:[[-2, -2], [1, 1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ ${2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ -1 2*t^2.29 + t^2.39 + 2*t^2.4 + t^2.41 + 2*t^3.49 + t^3.59 + t^3.61 + 3*t^4.59 + 2*t^4.68 + 6*t^4.69 + 2*t^4.7 + t^4.78 + 3*t^4.79 + 5*t^4.8 + 4*t^4.81 + t^4.82 + t^4.9 + t^4.91 + 4*t^5.79 + 3*t^5.88 + 5*t^5.89 + 3*t^5.9 + t^5.98 + 2*t^5.99 - t^6. + 3*t^6.01 + t^6.02 - t^6.12 + 4*t^6.88 + 4*t^6.98 + 13*t^6.99 + 3*t^7. + 2*t^7.07 + 9*t^7.08 + 14*t^7.09 + 11*t^7.1 + 2*t^7.11 + t^7.17 + 4*t^7.18 + 7*t^7.19 + 10*t^7.2 + 9*t^7.21 + 5*t^7.22 + t^7.23 + t^7.29 + 3*t^7.3 + t^7.31 + t^7.33 + t^7.39 + 6*t^8.08 + 5*t^8.18 + 13*t^8.19 + 5*t^8.2 + 3*t^8.27 + 9*t^8.28 + 5*t^8.29 + 11*t^8.3 + 3*t^8.31 + t^8.37 + 3*t^8.38 + t^8.39 - 3*t^8.4 + 4*t^8.42 + t^8.43 - t^8.5 - 4*t^8.51 - 3*t^8.52 - t^8.53 - t^8.6 - t^4.2/y - t^5.4/y - (2*t^6.49)/y - t^6.59/y - (2*t^6.6)/y - t^6.61/y + t^7.59/y + (2*t^7.68)/y + t^7.69/y + (2*t^7.7)/y + t^7.79/y + t^7.8/y + t^7.81/y + t^7.91/y + t^8.79/y + (2*t^8.88)/y - (2*t^8.89)/y + (2*t^8.9)/y - t^8.99/y - t^4.2*y - t^5.4*y - 2*t^6.49*y - t^6.59*y - 2*t^6.6*y - t^6.61*y + t^7.59*y + 2*t^7.68*y + t^7.69*y + 2*t^7.7*y + t^7.79*y + t^7.8*y + t^7.81*y + t^7.91*y + t^8.79*y + 2*t^8.88*y - 2*t^8.89*y + 2*t^8.9*y - t^8.99*y 2*g1*g2^2*t^2.29 + t^2.39/(g1^2*g2) + 2*t^2.4 + g1^2*g2*t^2.41 + 2*g1*g2^2*t^3.49 + t^3.59/(g1^2*g2) + g1^2*g2*t^3.61 + 3*g1^2*g2^4*t^4.59 + (2*g2*t^4.68)/g1 + 6*g1*g2^2*t^4.69 + 2*g1^3*g2^3*t^4.7 + t^4.78/(g1^4*g2^2) + (3*t^4.79)/(g1^2*g2) + 5*t^4.8 + 4*g1^2*g2*t^4.81 + g1^4*g2^2*t^4.82 + t^4.9/(g1^3*g2^3) + t^4.91/(g1*g2^2) + 4*g1^2*g2^4*t^5.79 + (3*g2*t^5.88)/g1 + 5*g1*g2^2*t^5.89 + 3*g1^3*g2^3*t^5.9 + t^5.98/(g1^4*g2^2) + (2*t^5.99)/(g1^2*g2) - t^6. + 3*g1^2*g2*t^6.01 + g1^4*g2^2*t^6.02 - (g1*t^6.12)/g2 + 4*g1^3*g2^6*t^6.88 + 4*g2^3*t^6.98 + 13*g1^2*g2^4*t^6.99 + 3*g1^4*g2^5*t^7. + (2*t^7.07)/g1^3 + (9*g2*t^7.08)/g1 + 14*g1*g2^2*t^7.09 + 11*g1^3*g2^3*t^7.1 + 2*g1^5*g2^4*t^7.11 + t^7.17/(g1^6*g2^3) + (4*t^7.18)/(g1^4*g2^2) + (7*t^7.19)/(g1^2*g2) + 10*t^7.2 + 9*g1^2*g2*t^7.21 + 5*g1^4*g2^2*t^7.22 + g1^6*g2^3*t^7.23 + t^7.29/(g1^5*g2^4) + (3*t^7.3)/(g1^3*g2^3) + t^7.31/(g1*g2^2) + g1^3*t^7.33 + t^7.39/(g1^6*g2^6) + 6*g1^3*g2^6*t^8.08 + 5*g2^3*t^8.18 + 13*g1^2*g2^4*t^8.19 + 5*g1^4*g2^5*t^8.2 + (3*t^8.27)/g1^3 + (9*g2*t^8.28)/g1 + 5*g1*g2^2*t^8.29 + 11*g1^3*g2^3*t^8.3 + 3*g1^5*g2^4*t^8.31 + t^8.37/(g1^6*g2^3) + (3*t^8.38)/(g1^4*g2^2) + t^8.39/(g1^2*g2) - 3*t^8.4 + 4*g1^4*g2^2*t^8.42 + g1^6*g2^3*t^8.43 - t^8.5/(g1^3*g2^3) - (4*t^8.51)/(g1*g2^2) - (3*g1*t^8.52)/g2 - g1^3*t^8.53 - t^8.6/(g1^4*g2^5) - t^4.2/y - t^5.4/y - (2*g1*g2^2*t^6.49)/y - t^6.59/(g1^2*g2*y) - (2*t^6.6)/y - (g1^2*g2*t^6.61)/y + (g1^2*g2^4*t^7.59)/y + (2*g2*t^7.68)/(g1*y) + (g1*g2^2*t^7.69)/y + (2*g1^3*g2^3*t^7.7)/y + t^7.79/(g1^2*g2*y) + t^7.8/y + (g1^2*g2*t^7.81)/y + t^7.91/(g1*g2^2*y) + (g1^2*g2^4*t^8.79)/y + (2*g2*t^8.88)/(g1*y) - (2*g1*g2^2*t^8.89)/y + (2*g1^3*g2^3*t^8.9)/y - t^8.99/(g1^2*g2*y) - t^4.2*y - t^5.4*y - 2*g1*g2^2*t^6.49*y - (t^6.59*y)/(g1^2*g2) - 2*t^6.6*y - g1^2*g2*t^6.61*y + g1^2*g2^4*t^7.59*y + (2*g2*t^7.68*y)/g1 + g1*g2^2*t^7.69*y + 2*g1^3*g2^3*t^7.7*y + (t^7.79*y)/(g1^2*g2) + t^7.8*y + g1^2*g2*t^7.81*y + (t^7.91*y)/(g1*g2^2) + g1^2*g2^4*t^8.79*y + (2*g2*t^8.88*y)/g1 - 2*g1*g2^2*t^8.89*y + 2*g1^3*g2^3*t^8.9*y - (t^8.99*y)/(g1^2*g2)


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
58370 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ 1.4121 1.6665 0.8473 [X:[], M:[0.7648, 1.1648], q:[0.4213, 0.3894], qb:[0.4139, 0.3754], phi:[0.4]] 2*t^2.29 + t^2.39 + t^2.4 + t^2.41 + 2*t^3.49 + t^3.59 + t^3.6 + t^3.61 + 3*t^4.59 + 2*t^4.68 + 4*t^4.69 + 2*t^4.7 + t^4.78 + 2*t^4.79 + 3*t^4.8 + 3*t^4.81 + t^4.82 + t^4.9 + t^4.91 + 4*t^5.79 + 3*t^5.88 + 5*t^5.89 + 3*t^5.9 + t^5.98 + 2*t^5.99 - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail