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
79565 Sp2s2nf1 ${}M_{1}S_{1}S_{2}$ + ${ }M_{2}S_{1}^{2}$ + ${ }M_{2}^{2}$ + ${ }q_{1}q_{2}S_{2}$ 2.3605 2.4543 0.9618 [X:[], M:[0.9, 1.0], q:[0.7, 0.7], qb:[], phi:[], S:[0.5, 0.6], Sb:[], A:[], Ab:[]] [X:[], M:[[0], [0]], q:[[-1], [1]], qb:[], phi:[], S:[[0], [0]], Sb:[], A:[], Ab:[]] 1 {a: 75537/32000, c: 78537/32000, M1: 9/10, M2: 1, q1: 7/10, q2: 7/10, S1: 1/2, S2: 3/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }M_{2}$, ${ }S_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }q_{1}^{2}S_{1}$, ${ }q_{1}q_{2}S_{1}$, ${ }q_{2}^{2}S_{1}$, ${ }q_{1}^{2}S_{1}$, ${ }q_{2}^{2}S_{1}$ ${}S_{1}^{4}$ 0 t^2.7 + t^3. + t^3.6 + t^4.2 + t^5.4 + 3*t^5.7 + t^6.3 + 3*t^6.6 + 2*t^6.9 + 4*t^7.2 + t^7.8 + t^8.1 + t^8.4 + 2*t^8.7 - t^4.5/y - t^4.8/y - (2*t^7.5)/y - (2*t^7.8)/y - (2*t^8.1)/y - (2*t^8.4)/y - t^4.5*y - t^4.8*y - 2*t^7.5*y - 2*t^7.8*y - 2*t^8.1*y - 2*t^8.4*y t^2.7 + t^3. + t^3.6 + t^4.2 + t^5.4 + t^5.7 + t^5.7/g1^2 + g1^2*t^5.7 + t^6.3 + 3*t^6.6 + 2*t^6.9 + 4*t^7.2 + t^7.8 + t^8.1 + t^8.4 + t^8.7/g1^2 + g1^2*t^8.7 - t^4.5/y - t^4.8/y - (2*t^7.5)/y - (2*t^7.8)/y - (2*t^8.1)/y - (2*t^8.4)/y - t^4.5*y - t^4.8*y - 2*t^7.5*y - 2*t^7.8*y - 2*t^8.1*y - 2*t^8.4*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
79624 ${}M_{1}S_{1}S_{2}$ + ${ }M_{2}S_{1}^{2}$ + ${ }M_{2}^{2}$ + ${ }q_{1}q_{2}S_{2}$ + ${ }M_{3}S_{2}^{2}$ 2.377 2.4833 0.9572 [X:[], M:[0.9, 1.0, 0.8], q:[0.7, 0.7], qb:[], phi:[], S:[0.5, 0.6], Sb:[], A:[], Ab:[]] t^2.4 + t^2.7 + t^3. + t^4.2 + t^4.8 + t^5.1 + 2*t^5.4 + 3*t^5.7 - t^4.5/y - t^4.8/y - t^4.5*y - t^4.8*y detail {a: 15213/6400, c: 15893/6400, M1: 9/10, M2: 1, M3: 4/5, q1: 7/10, q2: 7/10, S1: 1/2, S2: 3/5}


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
79513 Sp2s2nf1 ${}M_{1}S_{1}S_{2}$ + ${ }M_{2}S_{1}^{2}$ + ${ }M_{2}^{2}$ 2.3699 2.4822 0.9548 [X:[], M:[0.8802, 1.0], q:[0.6407, 0.6407], qb:[], phi:[], S:[0.5, 0.6198], Sb:[], A:[], Ab:[]] t^2.641 + t^3. + t^3.719 + t^3.844 + t^5.281 + 3*t^5.344 + 3*t^5.704 - 3*t^6. - t^4.5/y - t^4.859/y - t^4.5*y - t^4.859*y detail