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
61045 SU3adj1nf2 ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{2}\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ 0.9162 1.1065 0.828 [X:[1.5454, 1.5091, 1.4909, 1.4546], M:[1.0182, 0.9818, 0.9546], q:[0.1485, 0.1848], qb:[0.3061, 0.3606], phi:[0.5]] [X:[[0, -2], [-2, 0], [2, 0], [0, 2]], M:[[1, -1], [-1, 1], [0, 2]], q:[[-1, 1], [1, -1]], qb:[[1, 1], [-1, -1]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }X_{4}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }X_{3}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$ ${}$ -2 2*t^2.86 + t^2.95 + t^2.97 + t^3. + t^3.03 + t^3.05 + 2*t^4.36 + t^4.42 + t^4.45 + 2*t^4.47 + t^4.5 + 2*t^4.53 + t^4.55 + t^4.58 + 2*t^4.64 + 3*t^5.73 + 2*t^5.81 + 2*t^5.84 + t^5.86 + 2*t^5.89 + 2*t^5.92 + 2*t^5.95 + t^5.97 - 2*t^6. + t^6.03 + 2*t^6.05 - t^6.14 + 4*t^7.23 + t^7.25 + 2*t^7.28 + 2*t^7.31 + 4*t^7.34 + 3*t^7.36 + 7*t^7.39 + 4*t^7.42 + 3*t^7.45 + 3*t^7.47 + 7*t^7.5 + 3*t^7.53 + t^7.55 + 2*t^7.58 + 3*t^7.61 + t^7.64 + t^7.75 + 4*t^8.59 + 3*t^8.67 + 3*t^8.7 + 4*t^8.73 + 2*t^8.75 + 4*t^8.78 + 4*t^8.81 + 4*t^8.84 - 6*t^8.86 + 5*t^8.89 + 4*t^8.92 + t^8.95 - 3*t^8.97 - t^4.5/y - t^6./y - t^7.36/y + t^7.5/y + t^7.64/y + t^8.73/y + (2*t^8.81)/y + (2*t^8.84)/y - t^8.86/y + (2*t^8.89)/y + (3*t^8.92)/y + t^8.95/y - t^4.5*y - t^6.*y - t^7.36*y + t^7.5*y + t^7.64*y + t^8.73*y + 2*t^8.81*y + 2*t^8.84*y - t^8.86*y + 2*t^8.89*y + 3*t^8.92*y + t^8.95*y 2*g2^2*t^2.86 + (g2*t^2.95)/g1 + g1^2*t^2.97 + t^3. + t^3.03/g1^2 + (g1*t^3.05)/g2 + 2*g2^2*t^4.36 + g1*g2*t^4.42 + (g2*t^4.45)/g1 + 2*g1^2*t^4.47 + t^4.5 + (2*t^4.53)/g1^2 + (g1*t^4.55)/g2 + t^4.58/(g1*g2) + (2*t^4.64)/g2^2 + 3*g2^4*t^5.73 + (2*g2^3*t^5.81)/g1 + g1^2*g2^2*t^5.84 + (g2^3*t^5.84)/g1^3 + g2^2*t^5.86 + (2*g2^2*t^5.89)/g1^2 + 2*g1*g2*t^5.92 + g1^4*t^5.95 + (g2*t^5.95)/g1 + (g2*t^5.97)/g1^3 - 2*t^6. + (g1^3*t^6.03)/g2 + t^6.05/g1^4 + (g1*t^6.05)/g2 - t^6.14/g2^2 + (g1^3*t^6.16)/g2^3 - t^6.16/(g1^2*g2^2) + 4*g2^4*t^7.23 + g1^3*g2^3*t^7.25 + 2*g1*g2^3*t^7.28 + (2*g2^3*t^7.31)/g1 + 5*g1^2*g2^2*t^7.34 - (g2^3*t^7.34)/g1^3 + 3*g2^2*t^7.36 + g1^3*g2*t^7.39 + (6*g2^2*t^7.39)/g1^2 + 4*g1*g2*t^7.42 + 2*g1^4*t^7.45 + (g2*t^7.45)/g1 + 2*g1^2*t^7.47 + (g2*t^7.47)/g1^3 + 7*t^7.5 + (2*t^7.53)/g1^2 + (g1^3*t^7.53)/g2 + (2*t^7.55)/g1^4 - (g1*t^7.55)/g2 + (2*t^7.58)/(g1*g2) + (2*g1^2*t^7.61)/g2^2 + t^7.61/(g1^3*g2) + t^7.64/g2^2 - (g1^3*t^7.66)/g2^3 + t^7.66/(g1^2*g2^2) + t^7.75/(g1^3*g2^3) + 4*g2^6*t^8.59 + (3*g2^5*t^8.67)/g1 + g1^2*g2^4*t^8.7 + (2*g2^5*t^8.7)/g1^3 + 4*g2^4*t^8.73 - g1^3*g2^3*t^8.75 + (3*g2^4*t^8.75)/g1^2 + 3*g1*g2^3*t^8.78 + (g2^4*t^8.78)/g1^4 + g1^4*g2^2*t^8.81 + (3*g2^3*t^8.81)/g1 + 2*g1^2*g2^2*t^8.84 + (2*g2^3*t^8.84)/g1^3 - 7*g2^2*t^8.86 + (g2^3*t^8.86)/g1^5 + 2*g1^3*g2*t^8.89 + (3*g2^2*t^8.89)/g1^2 + g1^6*t^8.92 + g1*g2*t^8.92 + (2*g2^2*t^8.92)/g1^4 + 3*g1^4*t^8.95 - (2*g2*t^8.95)/g1 - 4*g1^2*t^8.97 + (g2*t^8.97)/g1^3 - t^4.5/y - t^6./y - (g2^2*t^7.36)/y + t^7.5/y + t^7.64/(g2^2*y) + (g2^4*t^8.73)/y + (2*g2^3*t^8.81)/(g1*y) + (2*g1^2*g2^2*t^8.84)/y - (g2^2*t^8.86)/y + (2*g2^2*t^8.89)/(g1^2*y) + (3*g1*g2*t^8.92)/y + (g2*t^8.95)/(g1*y) - (g1^2*t^8.97)/y + (g2*t^8.97)/(g1^3*y) - t^4.5*y - t^6.*y - g2^2*t^7.36*y + t^7.5*y + (t^7.64*y)/g2^2 + g2^4*t^8.73*y + (2*g2^3*t^8.81*y)/g1 + 2*g1^2*g2^2*t^8.84*y - g2^2*t^8.86*y + (2*g2^2*t^8.89*y)/g1^2 + 3*g1*g2*t^8.92*y + (g2*t^8.95*y)/g1 - g1^2*t^8.97*y + (g2*t^8.97*y)/g1^3


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
59069 SU3adj1nf2 ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{2}\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{1}M_{2}$ 0.9141 1.1016 0.8298 [X:[1.5, 1.5, 1.5, 1.5], M:[1.0, 1.0], q:[0.1667, 0.1667], qb:[0.3333, 0.3333], phi:[0.5]] 7*t^3. + 13*t^4.5 + 15*t^6. - t^4.5/y - t^6./y - t^4.5*y - t^6.*y detail {a: 117/128, c: 141/128, X1: 3/2, X2: 3/2, X3: 3/2, X4: 3/2, M1: 1, M2: 1, q1: 1/6, q2: 1/6, qb1: 1/3, qb2: 1/3, phi1: 1/2}