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
58859 SU3adj1nf2 ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ 0.9876 1.1933 0.8276 [X:[1.5364, 1.5088, 1.4912, 1.4636], M:[0.9636, 0.7456], q:[0.2422, 0.2699], qb:[0.2214, 0.2665], phi:[0.5]] [X:[[0, -3], [-2, 0], [2, 0], [0, 3]], M:[[0, 3], [1, 0]], q:[[-1, 1], [1, -2]], qb:[[1, 2], [-1, -1]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }X_{4}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }X_{3}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}M_{2}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}^{2}$ ${}$ -2 t^2.24 + 2*t^2.89 + t^2.97 + t^3. + t^3.03 + t^3.63 + t^3.76 + t^3.85 + 2*t^4.39 + 3*t^4.47 + t^4.5 + 2*t^4.53 + 2*t^4.61 + 3*t^5.13 + t^5.21 + t^5.24 + 3*t^5.26 + t^5.35 + 3*t^5.78 + 2*t^5.86 + t^5.89 + t^5.92 + t^5.95 - 2*t^6. + t^6.05 - t^6.11 - t^6.14 + t^6.49 + 2*t^6.52 + t^6.6 + 3*t^6.63 + t^6.65 + t^6.68 + 3*t^6.71 + 3*t^6.76 + t^6.79 + t^6.82 + 3*t^6.85 - t^6.87 + t^6.9 + t^6.93 + t^7.26 + 4*t^7.28 + 8*t^7.36 + 3*t^7.39 + 5*t^7.42 + 3*t^7.45 + 3*t^7.47 + 8*t^7.5 + 2*t^7.53 + 2*t^7.55 + 2*t^7.58 + t^7.61 + t^7.64 + t^7.69 - t^7.99 + 5*t^8.02 + 3*t^8.1 + t^8.13 + 4*t^8.15 - t^8.26 + t^8.29 + t^8.32 - t^8.35 - 2*t^8.37 - t^8.4 - t^8.43 + 4*t^8.67 + t^8.73 + 4*t^8.76 + 4*t^8.78 + t^8.81 + 2*t^8.84 + 4*t^8.86 - 6*t^8.89 + 3*t^8.92 + t^8.94 + 6*t^8.95 - 5*t^8.97 - t^4.5/y - t^6./y - t^6.74/y - t^7.39/y + t^7.5/y + t^7.61/y + (2*t^8.13)/y + t^8.21/y + (2*t^8.26)/y + t^8.78/y + (3*t^8.86)/y - t^8.89/y + (2*t^8.92)/y - (2*t^8.97)/y - t^4.5*y - t^6.*y - t^6.74*y - t^7.39*y + t^7.5*y + t^7.61*y + 2*t^8.13*y + t^8.21*y + 2*t^8.26*y + t^8.78*y + 3*t^8.86*y - t^8.89*y + 2*t^8.92*y - 2*t^8.97*y g1*t^2.24 + 2*g2^3*t^2.89 + g1^2*t^2.97 + t^3. + t^3.03/g1^2 + g1*g2^3*t^3.63 + t^3.76/g1 + (g1*t^3.85)/g2^3 + 2*g2^3*t^4.39 + 3*g1^2*t^4.47 + t^4.5 + (2*t^4.53)/g1^2 + (2*t^4.61)/g2^3 + 3*g1*g2^3*t^5.13 + g1^3*t^5.21 + g1*t^5.24 + (3*t^5.26)/g1 + (g1*t^5.35)/g2^3 + 3*g2^6*t^5.78 + 2*g1^2*g2^3*t^5.86 + g2^3*t^5.89 + (g2^3*t^5.92)/g1^2 + g1^4*t^5.95 - 2*t^6. + t^6.05/g1^4 - t^6.11/g2^3 - t^6.14/(g1^2*g2^3) + g1^3*g2^6*t^6.49 + 2*g1*g2^6*t^6.52 + g1^3*g2^3*t^6.6 + 3*g1*g2^3*t^6.63 + (g2^3*t^6.65)/g1 + (g2^3*t^6.68)/g1^3 + 3*g1^3*t^6.71 + (3*t^6.76)/g1 + t^6.79/g1^3 + (g1^3*t^6.82)/g2^3 + (3*g1*t^6.85)/g2^3 - t^6.87/(g1*g2^3) + t^6.9/(g1^3*g2^3) + (g1^3*t^6.93)/g2^6 + g1^2*g2^6*t^7.26 + 4*g2^6*t^7.28 + 8*g1^2*g2^3*t^7.36 + 3*g2^3*t^7.39 + (5*g2^3*t^7.42)/g1^2 + 3*g1^4*t^7.45 + 3*g1^2*t^7.47 + 8*t^7.5 + (2*t^7.53)/g1^2 + (2*t^7.55)/g1^4 + (2*g1^2*t^7.58)/g2^3 + t^7.61/g2^3 + t^7.64/(g1^2*g2^3) + (g1^2*t^7.69)/g2^6 - g1^3*g2^6*t^7.99 + 5*g1*g2^6*t^8.02 + 3*g1^3*g2^3*t^8.1 + g1*g2^3*t^8.13 + (4*g2^3*t^8.15)/g1 + g1^5*t^8.18 - (g2^3*t^8.18)/g1^3 - t^8.26/g1 + t^8.29/g1^3 + (g1^3*t^8.32)/g2^3 - (g1*t^8.35)/g2^3 - (2*t^8.37)/(g1*g2^3) - t^8.4/(g1^3*g2^3) - (g1^3*t^8.43)/g2^6 + 4*g2^9*t^8.67 + g1^4*g2^6*t^8.73 + 4*g1^2*g2^6*t^8.76 + 4*g2^6*t^8.78 + (g2^6*t^8.81)/g1^2 + 2*g1^4*g2^3*t^8.84 + 4*g1^2*g2^3*t^8.86 - 6*g2^3*t^8.89 + g1^6*t^8.92 + (2*g2^3*t^8.92)/g1^2 + (g2^3*t^8.94)/g1^4 + 6*g1^4*t^8.95 - 5*g1^2*t^8.97 - t^4.5/y - t^6./y - (g1*t^6.74)/y - (g2^3*t^7.39)/y + t^7.5/y + t^7.61/(g2^3*y) + (2*g1*g2^3*t^8.13)/y + (g1^3*t^8.21)/y + (2*t^8.26)/(g1*y) + (g2^6*t^8.78)/y + (3*g1^2*g2^3*t^8.86)/y - (g2^3*t^8.89)/y + (2*g2^3*t^8.92)/(g1^2*y) - (2*g1^2*t^8.97)/y - t^4.5*y - t^6.*y - g1*t^6.74*y - g2^3*t^7.39*y + t^7.5*y + (t^7.61*y)/g2^3 + 2*g1*g2^3*t^8.13*y + g1^3*t^8.21*y + (2*t^8.26*y)/g1 + g2^6*t^8.78*y + 3*g1^2*g2^3*t^8.86*y - g2^3*t^8.89*y + (2*g2^3*t^8.92*y)/g1^2 - 2*g1^2*t^8.97*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
57512 SU3adj1nf2 ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{1}^{2}q_{2}$ 0.9877 1.1935 0.8275 [X:[1.535, 1.5082, 1.4918, 1.465], M:[0.965, 0.7415], q:[0.2439, 0.2706], qb:[0.2211, 0.2643], phi:[0.5]] t^2.22 + 2*t^2.9 + t^2.98 + t^3. + t^3.02 + t^3.62 + t^3.75 + t^3.86 + 2*t^4.4 + t^4.45 + 2*t^4.48 + t^4.5 + 2*t^4.52 + 2*t^4.6 + 3*t^5.12 + t^5.2 + t^5.22 + 2*t^5.25 + t^5.28 + t^5.36 + 3*t^5.79 + t^5.84 + t^5.87 + t^5.9 + t^5.92 + t^5.95 + t^5.97 - 3*t^6. - t^4.5/y - t^6./y - t^4.5*y - t^6.*y detail