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
1210 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ 0.6635 0.8374 0.7923 [M:[1.1924, 0.7824, 0.8076, 0.8076, 0.8201, 0.795], q:[0.8013, 0.4164], qb:[0.3912, 0.8013], phi:[0.3975]] [M:[[-6], [-14], [6], [6], [16], [-4]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$ ${}\phi_{1}\tilde{q}_{2}^{2}$ 0 t^2.347 + 2*t^2.385 + 2*t^2.423 + t^2.46 + t^3.577 + t^3.653 + t^3.691 + t^4.694 + 2*t^4.732 + 5*t^4.77 + 6*t^4.808 + 5*t^4.845 + 2*t^4.883 + t^4.921 + 2*t^6.038 + 3*t^6.076 + 3*t^6.113 + t^6.151 + t^7.041 + 2*t^7.079 + 4*t^7.117 + 8*t^7.155 + 9*t^7.192 + 9*t^7.23 + 8*t^7.268 + 5*t^7.306 + 3*t^7.344 + 2*t^7.381 - 2*t^8.309 - 4*t^8.347 - 5*t^8.385 - 3*t^8.423 + 2*t^8.46 + 7*t^8.498 + 6*t^8.536 + 3*t^8.574 + t^8.612 - t^4.192/y - t^6.54/y - (2*t^6.577)/y - t^6.615/y - t^6.653/y + (3*t^7.732)/y + (4*t^7.77)/y + (7*t^7.808)/y + (4*t^7.845)/y + (2*t^7.883)/y - t^8.887/y - t^8.924/y - (2*t^8.962)/y - t^4.192*y - t^6.54*y - 2*t^6.577*y - t^6.615*y - t^6.653*y + 3*t^7.732*y + 4*t^7.77*y + 7*t^7.808*y + 4*t^7.845*y + 2*t^7.883*y - t^8.887*y - t^8.924*y - 2*t^8.962*y t^2.347/g1^14 + (2*t^2.385)/g1^4 + 2*g1^6*t^2.423 + g1^16*t^2.46 + t^3.577/g1^6 + g1^14*t^3.653 + g1^24*t^3.691 + t^4.694/g1^28 + (2*t^4.732)/g1^18 + (5*t^4.77)/g1^8 + 6*g1^2*t^4.808 + 5*g1^12*t^4.845 + 2*g1^22*t^4.883 + g1^32*t^4.921 + 2*g1^10*t^6.038 + 3*g1^20*t^6.076 + 3*g1^30*t^6.113 + g1^40*t^6.151 + t^7.041/g1^42 + (2*t^7.079)/g1^32 + (4*t^7.117)/g1^22 + (8*t^7.155)/g1^12 + (9*t^7.192)/g1^2 + 9*g1^8*t^7.23 + 8*g1^18*t^7.268 + 5*g1^28*t^7.306 + 3*g1^38*t^7.344 + 2*g1^48*t^7.381 - (2*t^8.309)/g1^24 - (4*t^8.347)/g1^14 - (5*t^8.385)/g1^4 - 3*g1^6*t^8.423 + 2*g1^16*t^8.46 + 7*g1^26*t^8.498 + 6*g1^36*t^8.536 + 3*g1^46*t^8.574 + g1^56*t^8.612 - t^4.192/(g1^2*y) - t^6.54/(g1^16*y) - (2*t^6.577)/(g1^6*y) - (g1^4*t^6.615)/y - (g1^14*t^6.653)/y + (3*t^7.732)/(g1^18*y) + (4*t^7.77)/(g1^8*y) + (7*g1^2*t^7.808)/y + (4*g1^12*t^7.845)/y + (2*g1^22*t^7.883)/y - t^8.887/(g1^30*y) - t^8.924/(g1^20*y) - (2*t^8.962)/(g1^10*y) - (t^4.192*y)/g1^2 - (t^6.54*y)/g1^16 - (2*t^6.577*y)/g1^6 - g1^4*t^6.615*y - g1^14*t^6.653*y + (3*t^7.732*y)/g1^18 + (4*t^7.77*y)/g1^8 + 7*g1^2*t^7.808*y + 4*g1^12*t^7.845*y + 2*g1^22*t^7.883*y - (t^8.887*y)/g1^30 - (t^8.924*y)/g1^20 - (2*t^8.962*y)/g1^10


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
2244 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{7}$ 0.6465 0.8092 0.799 [M:[1.2006, 0.8015, 0.7994, 0.7994, 0.7983, 0.8004, 1.1985], q:[0.7999, 0.3986], qb:[0.4008, 0.7999], phi:[0.4002]] t^2.395 + 2*t^2.398 + 2*t^2.401 + t^3.592 + 2*t^3.595 + t^3.602 + t^4.79 + 2*t^4.793 + 5*t^4.796 + 5*t^4.799 + 3*t^4.803 + t^5.987 + 4*t^5.99 + 5*t^5.994 + 3*t^5.997 - t^6. - t^4.201/y - t^4.201*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
737 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ 0.6467 0.8082 0.8002 [M:[1.1947, 0.7877, 0.8053, 0.8053, 0.814], q:[0.8009, 0.4114], qb:[0.3939, 0.8009], phi:[0.3982]] t^2.363 + t^2.389 + 2*t^2.416 + t^2.442 + t^3.584 + t^3.611 + t^3.637 + t^3.663 + t^4.726 + t^4.753 + 3*t^4.779 + 4*t^4.805 + 4*t^4.832 + 2*t^4.858 + t^4.884 + t^6. - t^4.195/y - t^4.195*y detail