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
2719 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ 0.6575 0.8468 0.7765 [M:[1.1387, 0.7226, 0.75, 0.8613], q:[0.75, 0.3613], qb:[0.5, 0.3887], phi:[0.5]] [M:[[1], [-2], [0], [-1]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{1}q_{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}^{2}\tilde{q}_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$ ${}M_{4}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ 1 t^2.168 + 2*t^2.25 + t^2.584 + t^2.666 + t^3. + t^3.334 + t^3.416 + t^3.668 + t^3.75 + t^4.084 + t^4.166 + t^4.336 + 2*t^4.418 + 4*t^4.5 + t^4.752 + 3*t^4.834 + 2*t^4.916 + 2*t^5.168 + 3*t^5.25 + t^5.332 + t^5.502 + 3*t^5.584 + 2*t^5.666 + t^5.836 + 3*t^5.918 + t^6. + 2*t^6.252 + 3*t^6.334 + t^6.416 + t^6.504 + 2*t^6.586 + 6*t^6.668 + 6*t^6.75 + t^6.832 + t^6.92 + 4*t^7.002 + 5*t^7.084 + 2*t^7.166 + 3*t^7.336 + 5*t^7.418 + 4*t^7.5 + t^7.582 + t^7.67 + 5*t^7.752 + 5*t^7.834 + 2*t^7.916 + t^7.998 + t^8.004 + 3*t^8.086 + 5*t^8.168 + 2*t^8.42 + 5*t^8.502 + 2*t^8.584 - t^8.666 + t^8.672 + 2*t^8.754 + 7*t^8.836 + 8*t^8.918 - t^4.5/y - t^6.668/y - t^6.75/y + (2*t^7.418)/y + t^7.5/y + t^7.752/y + (3*t^7.834)/y + (2*t^7.916)/y + t^8.168/y + (4*t^8.25)/y + t^8.332/y + t^8.502/y + (4*t^8.584)/y + (3*t^8.666)/y + (3*t^8.918)/y - t^4.5*y - t^6.668*y - t^6.75*y + 2*t^7.418*y + t^7.5*y + t^7.752*y + 3*t^7.834*y + 2*t^7.916*y + t^8.168*y + 4*t^8.25*y + t^8.332*y + t^8.502*y + 4*t^8.584*y + 3*t^8.666*y + 3*t^8.918*y t^2.168/g1^2 + 2*t^2.25 + t^2.584/g1 + g1*t^2.666 + t^3. + t^3.334/g1 + g1*t^3.416 + t^3.668/g1^2 + t^3.75 + t^4.084/g1 + g1*t^4.166 + t^4.336/g1^4 + (2*t^4.418)/g1^2 + 4*t^4.5 + t^4.752/g1^3 + (3*t^4.834)/g1 + 2*g1*t^4.916 + (2*t^5.168)/g1^2 + 3*t^5.25 + g1^2*t^5.332 + t^5.502/g1^3 + (3*t^5.584)/g1 + 2*g1*t^5.666 + t^5.836/g1^4 + (3*t^5.918)/g1^2 + t^6. + (2*t^6.252)/g1^3 + (3*t^6.334)/g1 + g1*t^6.416 + t^6.504/g1^6 + (2*t^6.586)/g1^4 + (6*t^6.668)/g1^2 + 6*t^6.75 + g1^2*t^6.832 + t^6.92/g1^5 + (4*t^7.002)/g1^3 + (5*t^7.084)/g1 + 2*g1*t^7.166 + (3*t^7.336)/g1^4 + (5*t^7.418)/g1^2 + 4*t^7.5 + g1^2*t^7.582 + t^7.67/g1^5 + (5*t^7.752)/g1^3 + (5*t^7.834)/g1 + 2*g1*t^7.916 + g1^3*t^7.998 + t^8.004/g1^6 + (3*t^8.086)/g1^4 + (5*t^8.168)/g1^2 + (2*t^8.42)/g1^5 + (5*t^8.502)/g1^3 + (2*t^8.584)/g1 - g1*t^8.666 + t^8.672/g1^8 + (2*t^8.754)/g1^6 + (7*t^8.836)/g1^4 + (8*t^8.918)/g1^2 - t^4.5/y - t^6.668/(g1^2*y) - t^6.75/y + (2*t^7.418)/(g1^2*y) + t^7.5/y + t^7.752/(g1^3*y) + (3*t^7.834)/(g1*y) + (2*g1*t^7.916)/y + t^8.168/(g1^2*y) + (4*t^8.25)/y + (g1^2*t^8.332)/y + t^8.502/(g1^3*y) + (4*t^8.584)/(g1*y) + (3*g1*t^8.666)/y + (3*t^8.918)/(g1^2*y) - t^4.5*y - (t^6.668*y)/g1^2 - t^6.75*y + (2*t^7.418*y)/g1^2 + t^7.5*y + (t^7.752*y)/g1^3 + (3*t^7.834*y)/g1 + 2*g1*t^7.916*y + (t^8.168*y)/g1^2 + 4*t^8.25*y + g1^2*t^8.332*y + (t^8.502*y)/g1^3 + (4*t^8.584*y)/g1 + 3*g1*t^8.666*y + (3*t^8.918*y)/g1^2


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
3232 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ 0.676 0.8792 0.769 [M:[1.125, 0.75, 0.75, 0.875, 0.75], q:[0.75, 0.375], qb:[0.5, 0.375], phi:[0.5]] 4*t^2.25 + 2*t^2.625 + t^3. + 2*t^3.375 + t^3.75 + 2*t^4.125 + 11*t^4.5 + 8*t^4.875 + 7*t^5.25 + 8*t^5.625 + 3*t^6. - t^4.5/y - t^4.5*y detail {a: 2769/4096, c: 3601/4096, M1: 9/8, M2: 3/4, M3: 3/4, M4: 7/8, M5: 3/4, q1: 3/4, q2: 3/8, qb1: 1/2, qb2: 3/8, phi1: 1/2}
3233 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ 0.6766 0.8814 0.7676 [M:[1.1387, 0.7226, 0.75, 0.8613, 0.75], q:[0.75, 0.3613], qb:[0.5, 0.3887], phi:[0.5]] t^2.168 + 3*t^2.25 + t^2.584 + t^2.666 + t^3. + t^3.334 + t^3.416 + t^3.668 + t^4.084 + t^4.166 + t^4.336 + 3*t^4.418 + 7*t^4.5 + t^4.752 + 4*t^4.834 + 3*t^4.916 + 2*t^5.168 + 4*t^5.25 + t^5.332 + t^5.502 + 4*t^5.584 + 3*t^5.666 + t^5.836 + 3*t^5.918 - t^6. - t^4.5/y - t^4.5*y detail
3234 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ 0.6703 0.8704 0.7701 [M:[1.1508, 0.6985, 0.75, 0.8492, 0.8492], q:[0.75, 0.3492], qb:[0.5, 0.4008], phi:[0.5]] t^2.095 + 2*t^2.25 + 2*t^2.548 + t^2.702 + t^3. + t^3.298 + t^3.595 + t^3.75 + t^4.048 + t^4.191 + t^4.202 + 2*t^4.345 + 4*t^4.5 + 2*t^4.643 + 5*t^4.798 + 2*t^4.952 + 4*t^5.095 + 4*t^5.25 + t^5.393 + t^5.405 + 3*t^5.548 + t^5.691 + 4*t^5.845 - t^4.5/y - t^4.5*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
1718 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ 0.6458 0.8255 0.7823 [M:[1.1253, 0.7495, 0.75], q:[0.75, 0.3747], qb:[0.5, 0.3753], phi:[0.5]] t^2.248 + 2*t^2.25 + t^2.626 + t^3. + t^3.374 + 2*t^3.376 + t^3.748 + t^3.75 + t^4.124 + t^4.126 + t^4.497 + 2*t^4.498 + 4*t^4.5 + t^4.874 + 2*t^4.876 + t^5.248 + 2*t^5.25 + t^5.252 + t^5.623 + 3*t^5.624 + 4*t^5.626 + t^5.997 + 2*t^5.998 - t^4.5/y - t^4.5*y detail