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
57908 SU3adj1nf2 ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}^{2}$ + ${ }q_{1}\tilde{q}_{1}X_{2}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ 1.2649 1.4774 0.8562 [X:[1.2, 1.4], M:[1.0], q:[0.3455, 0.6273], qb:[0.2545, 0.3727], phi:[0.4]] [X:[[0], [0]], M:[[0]], q:[[2], [-1]], qb:[[-2], [1]], phi:[[0]]] 1 {a: 222627/176000, c: 260027/176000, X1: 6/5, X2: 7/5, M1: 1, q1: 19/55, q2: 69/110, qb1: 14/55, qb2: 41/110, phi1: 2/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }X_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}X_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$ ${2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ 2 t^2.15 + t^2.65 + 2*t^3. + t^3.35 + 2*t^3.6 + 2*t^3.85 + 4*t^4.2 + t^4.31 + t^4.55 + t^4.8 + 2*t^5.05 + 2*t^5.15 + t^5.29 + 2*t^5.4 + t^5.51 + t^5.65 + 2*t^5.75 + t^5.89 + 2*t^6. + 3*t^6.25 + 5*t^6.35 + t^6.46 + 2*t^6.49 + 4*t^6.6 + 3*t^6.71 + 4*t^6.85 + 3*t^6.95 + 10*t^7.2 + 2*t^7.31 + 3*t^7.45 + 6*t^7.55 + t^7.66 + 4*t^7.69 + 5*t^7.8 + 3*t^7.91 + t^7.94 + 8*t^8.05 + t^8.15 + 14*t^8.4 + 4*t^8.51 + t^8.54 + t^8.62 + t^8.65 + 6*t^8.75 + 3*t^8.86 + 7*t^8.89 - t^4.2/y - t^5.4/y - t^6.35/y - t^6.85/y - t^7.2/y - t^7.55/y - t^8.05/y + (2*t^8.15)/y - (3*t^8.4)/y + (2*t^8.65)/y + t^8.75/y - t^4.2*y - t^5.4*y - t^6.35*y - t^6.85*y - t^7.2*y - t^7.55*y - t^8.05*y + 2*t^8.15*y - 3*t^8.4*y + 2*t^8.65*y + t^8.75*y g1^3*t^2.15 + t^2.65/g1^3 + 2*t^3. + g1^3*t^3.35 + 2*t^3.6 + (2*t^3.85)/g1^3 + 4*t^4.2 + g1^6*t^4.31 + g1^3*t^4.55 + t^4.8 + (2*t^5.05)/g1^3 + 2*g1^3*t^5.15 + t^5.29/g1^6 + 2*t^5.4 + g1^6*t^5.51 + t^5.65/g1^3 + 2*g1^3*t^5.75 + t^5.89/g1^6 + 2*t^6. + (3*t^6.25)/g1^3 + 5*g1^3*t^6.35 + g1^9*t^6.46 + (2*t^6.49)/g1^6 + 4*t^6.6 + 3*g1^6*t^6.71 + (4*t^6.85)/g1^3 + 3*g1^3*t^6.95 + 10*t^7.2 + 2*g1^6*t^7.31 + (3*t^7.45)/g1^3 + 6*g1^3*t^7.55 + g1^9*t^7.66 + (4*t^7.69)/g1^6 + 5*t^7.8 + 3*g1^6*t^7.91 + t^7.94/g1^9 + (8*t^8.05)/g1^3 + g1^3*t^8.15 + 14*t^8.4 + 4*g1^6*t^8.51 + t^8.54/g1^9 + g1^12*t^8.62 + t^8.65/g1^3 + 6*g1^3*t^8.75 + 3*g1^9*t^8.86 + (7*t^8.89)/g1^6 - t^4.2/y - t^5.4/y - (g1^3*t^6.35)/y - t^6.85/(g1^3*y) - t^7.2/y - (g1^3*t^7.55)/y - t^8.05/(g1^3*y) + (2*g1^3*t^8.15)/y - (3*t^8.4)/y + (2*t^8.65)/(g1^3*y) + (g1^3*t^8.75)/y - t^4.2*y - t^5.4*y - g1^3*t^6.35*y - (t^6.85*y)/g1^3 - t^7.2*y - g1^3*t^7.55*y - (t^8.05*y)/g1^3 + 2*g1^3*t^8.15*y - 3*t^8.4*y + (2*t^8.65*y)/g1^3 + g1^3*t^8.75*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
61027 ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}^{2}$ + ${ }q_{1}\tilde{q}_{1}X_{2}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ 1.2851 1.5156 0.8479 [X:[1.2, 1.4], M:[1.0, 0.7118], q:[0.3412, 0.6294], qb:[0.2588, 0.3706], phi:[0.4]] 2*t^2.14 + t^2.66 + 2*t^3. + t^3.34 + 2*t^3.6 + t^3.86 + 4*t^4.2 + 3*t^4.27 + t^4.54 + 2*t^4.8 + 2*t^5.06 + 4*t^5.14 + t^5.33 + 2*t^5.4 + 2*t^5.47 + t^5.66 + 4*t^5.74 + t^5.93 + 2*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail


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
57294 SU3adj1nf2 ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}^{2}$ + ${ }q_{1}\tilde{q}_{1}X_{2}$ 1.3133 1.5258 0.8607 [X:[1.2, 1.4], M:[1.0], q:[0.3, 0.5], qb:[0.3, 0.5], phi:[0.4]] 2*t^2.4 + 2*t^3. + 4*t^3.6 + 3*t^4.2 + 2*t^4.5 + 5*t^4.8 + 2*t^5.1 + 3*t^5.4 + 2*t^5.7 + 7*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail {a: 5253/4000, c: 6103/4000, X1: 6/5, X2: 7/5, M1: 1, q1: 3/10, q2: 1/2, qb1: 3/10, qb2: 1/2, phi1: 2/5}