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
57942 SU3adj1nf2 ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ 1.39 1.606 0.8656 [X:[1.2727], M:[0.9091], q:[0.3361, 0.4683], qb:[0.3912, 0.6226], phi:[0.3636]] [X:[[0]], M:[[0]], q:[[2], [-1]], qb:[[-2], [1]], phi:[[0]]] 1 {a: 162813/117128, c: 94051/58564, X1: 14/11, M1: 10/11, q1: 122/363, q2: 170/363, qb1: 142/363, qb2: 226/363, phi1: 4/11}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ ${}\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}X_{1}$ 1 t^2.18 + t^2.58 + t^2.73 + t^2.88 + 2*t^3.27 + t^3.67 + t^3.82 + t^3.97 + 3*t^4.36 + t^4.51 + 2*t^4.76 + 2*t^4.91 + 2*t^5.06 + t^5.16 + t^5.31 + 5*t^5.45 + t^5.6 + t^5.75 + 3*t^5.85 + t^6. + 3*t^6.15 + t^6.25 + t^6.3 + t^6.4 + 8*t^6.55 + 2*t^6.69 + t^6.79 + t^6.84 + 6*t^6.94 + 5*t^7.09 + 5*t^7.24 + 3*t^7.34 + t^7.39 + 3*t^7.49 + 10*t^7.64 + t^7.74 + 3*t^7.79 + t^7.88 + 2*t^7.93 + 7*t^8.03 + 5*t^8.18 + 7*t^8.33 + 3*t^8.43 + 3*t^8.48 + t^8.58 + t^8.63 + 12*t^8.73 + t^8.83 + 4*t^8.88 + 2*t^8.98 - t^4.09/y - t^5.18/y - t^6.27/y - t^6.67/y - t^6.82/y - t^6.97/y - (2*t^7.36)/y + t^8.31/y + t^8.6/y + t^8.85/y - t^4.09*y - t^5.18*y - t^6.27*y - t^6.67*y - t^6.82*y - t^6.97*y - 2*t^7.36*y + t^8.31*y + t^8.6*y + t^8.85*y t^2.18 + t^2.58/g1^3 + t^2.73 + g1^3*t^2.88 + 2*t^3.27 + t^3.67/g1^3 + t^3.82 + g1^3*t^3.97 + 3*t^4.36 + g1^3*t^4.51 + (2*t^4.76)/g1^3 + 2*t^4.91 + 2*g1^3*t^5.06 + t^5.16/g1^6 + t^5.31/g1^3 + 5*t^5.45 + g1^3*t^5.6 + g1^6*t^5.75 + (3*t^5.85)/g1^3 + t^6. + 3*g1^3*t^6.15 + t^6.25/g1^6 + g1^6*t^6.3 + t^6.4/g1^3 + 8*t^6.55 + 2*g1^3*t^6.69 + t^6.79/g1^6 + g1^6*t^6.84 + (6*t^6.94)/g1^3 + 5*t^7.09 + 5*g1^3*t^7.24 + (3*t^7.34)/g1^6 + g1^6*t^7.39 + (3*t^7.49)/g1^3 + 10*t^7.64 + t^7.74/g1^9 + 3*g1^3*t^7.79 + t^7.88/g1^6 + 2*g1^6*t^7.93 + (7*t^8.03)/g1^3 + 5*t^8.18 + 7*g1^3*t^8.33 + (3*t^8.43)/g1^6 + 3*g1^6*t^8.48 + t^8.58/g1^3 + g1^9*t^8.63 + 12*t^8.73 + t^8.83/g1^9 + 4*g1^3*t^8.88 + (2*t^8.98)/g1^6 - t^4.09/y - t^5.18/y - t^6.27/y - t^6.67/(g1^3*y) - t^6.82/y - (g1^3*t^6.97)/y - (2*t^7.36)/y + t^8.31/(g1^3*y) + (g1^3*t^8.6)/y + t^8.85/(g1^3*y) - t^4.09*y - t^5.18*y - t^6.27*y - (t^6.67*y)/g1^3 - t^6.82*y - g1^3*t^6.97*y - 2*t^7.36*y + (t^8.31*y)/g1^3 + g1^3*t^8.6*y + (t^8.85*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
61184 ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{2}X_{1}$ 1.4099 1.6429 0.8582 [X:[1.2727], M:[0.9091, 0.7273], q:[0.3361, 0.4683], qb:[0.3912, 0.6226], phi:[0.3636]] 2*t^2.18 + t^2.58 + t^2.73 + t^2.88 + 2*t^3.27 + t^3.67 + t^3.97 + 5*t^4.36 + t^4.51 + 3*t^4.76 + 3*t^4.91 + 3*t^5.06 + t^5.16 + t^5.31 + 7*t^5.45 + t^5.6 + t^5.75 + 4*t^5.85 - t^4.09/y - t^5.18/y - t^4.09*y - t^5.18*y detail {a: 330279/234256, c: 192425/117128, X1: 14/11, M1: 10/11, M2: 8/11, q1: 122/363, q2: 170/363, qb1: 142/363, qb2: 226/363, phi1: 4/11}


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
57302 SU3adj1nf2 ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ 1.4334 1.623 0.8832 [X:[1.3613], M:[0.7984], q:[0.4354, 0.5847], qb:[0.4469, 0.6169], phi:[0.3194]] t^2.395 + t^2.647 + t^2.874 + t^3.095 + t^3.157 + t^3.605 + t^4.053 + t^4.084 + t^4.115 + 2*t^4.563 + t^4.79 + t^5.011 + t^5.042 + t^5.073 + t^5.269 + t^5.293 + t^5.324 + t^5.49 + 2*t^5.521 + t^5.741 + t^5.748 + t^5.773 + t^5.804 + t^5.969 - 2*t^6. - t^3.958/y - t^4.916/y - t^3.958*y - t^4.916*y detail