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
46582 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ 0.6977 0.8709 0.8011 [M:[0.6748, 1.1084, 0.7832, 0.8916], q:[0.7771, 0.5481], qb:[0.4519, 0.4397], phi:[0.4458]] [M:[[-12], [4], [-8], [-4]], q:[[1], [11]], qb:[[-11], [7]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }M_{3}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ ${}M_{1}\phi_{1}\tilde{q}_{2}^{2}$ -1 t^2.024 + t^2.35 + 2*t^2.675 + t^2.963 + t^3. + t^3.687 + t^3.976 + t^4.012 + 2*t^4.049 + t^4.301 + t^4.337 + t^4.374 + t^4.626 + 3*t^4.699 + t^4.988 + 3*t^5.024 + t^5.313 + 4*t^5.35 + 2*t^5.638 + t^5.675 + t^5.927 - t^6. + t^6.037 + 2*t^6.073 - t^6.289 + 3*t^6.362 + 2*t^6.398 + 3*t^6.65 + 3*t^6.687 + 5*t^6.723 + t^6.939 + 3*t^6.976 + 2*t^7.012 + 4*t^7.049 + t^7.264 + t^7.301 - t^7.337 + 5*t^7.374 + t^7.59 - t^7.626 + t^7.663 + 5*t^7.699 + t^7.736 + 2*t^7.988 + 5*t^8.024 + t^8.061 + 3*t^8.097 + t^8.277 + 2*t^8.313 - t^8.35 + 2*t^8.386 + 2*t^8.423 + 3*t^8.602 - 2*t^8.638 - 3*t^8.675 + 3*t^8.711 + 6*t^8.748 + t^8.89 + t^8.927 - 3*t^8.963 - t^4.337/y - t^6.362/y - t^6.687/y - t^7.012/y + t^7.374/y + t^7.663/y + (2*t^7.699)/y + (2*t^7.988)/y + (3*t^8.024)/y + (2*t^8.313)/y + (2*t^8.35)/y - t^8.386/y + (2*t^8.638)/y + (2*t^8.675)/y + t^8.963/y - t^4.337*y - t^6.362*y - t^6.687*y - t^7.012*y + t^7.374*y + t^7.663*y + 2*t^7.699*y + 2*t^7.988*y + 3*t^8.024*y + 2*t^8.313*y + 2*t^8.35*y - t^8.386*y + 2*t^8.638*y + 2*t^8.675*y + t^8.963*y t^2.024/g1^12 + t^2.35/g1^8 + (2*t^2.675)/g1^4 + g1^18*t^2.963 + t^3. + t^3.687/g1^10 + g1^12*t^3.976 + t^4.012/g1^6 + (2*t^4.049)/g1^24 + g1^16*t^4.301 + t^4.337/g1^2 + t^4.374/g1^20 + g1^20*t^4.626 + (3*t^4.699)/g1^16 + g1^6*t^4.988 + (3*t^5.024)/g1^12 + g1^10*t^5.313 + (4*t^5.35)/g1^8 + 2*g1^14*t^5.638 + t^5.675/g1^4 + g1^36*t^5.927 - t^6. + t^6.037/g1^18 + (2*t^6.073)/g1^36 - g1^22*t^6.289 + (3*t^6.362)/g1^14 + (2*t^6.398)/g1^32 + 3*g1^8*t^6.65 + (3*t^6.687)/g1^10 + (5*t^6.723)/g1^28 + g1^30*t^6.939 + 3*g1^12*t^6.976 + (2*t^7.012)/g1^6 + (4*t^7.049)/g1^24 + g1^34*t^7.264 + g1^16*t^7.301 - t^7.337/g1^2 + (5*t^7.374)/g1^20 + g1^38*t^7.59 - g1^20*t^7.626 + g1^2*t^7.663 + (5*t^7.699)/g1^16 + t^7.736/g1^34 + 2*g1^6*t^7.988 + (5*t^8.024)/g1^12 + t^8.061/g1^30 + (3*t^8.097)/g1^48 + g1^28*t^8.277 + 2*g1^10*t^8.313 - t^8.35/g1^8 + (2*t^8.386)/g1^26 + (2*t^8.423)/g1^44 + 3*g1^32*t^8.602 - 2*g1^14*t^8.638 - (3*t^8.675)/g1^4 + (3*t^8.711)/g1^22 + (6*t^8.748)/g1^40 + g1^54*t^8.89 + g1^36*t^8.927 - 3*g1^18*t^8.963 - t^4.337/(g1^2*y) - t^6.362/(g1^14*y) - t^6.687/(g1^10*y) - t^7.012/(g1^6*y) + t^7.374/(g1^20*y) + (g1^2*t^7.663)/y + (2*t^7.699)/(g1^16*y) + (2*g1^6*t^7.988)/y + (3*t^8.024)/(g1^12*y) + (2*g1^10*t^8.313)/y + (2*t^8.35)/(g1^8*y) - t^8.386/(g1^26*y) + (2*g1^14*t^8.638)/y + (2*t^8.675)/(g1^4*y) + (g1^18*t^8.963)/y - (t^4.337*y)/g1^2 - (t^6.362*y)/g1^14 - (t^6.687*y)/g1^10 - (t^7.012*y)/g1^6 + (t^7.374*y)/g1^20 + g1^2*t^7.663*y + (2*t^7.699*y)/g1^16 + 2*g1^6*t^7.988*y + (3*t^8.024*y)/g1^12 + 2*g1^10*t^8.313*y + (2*t^8.35*y)/g1^8 - (t^8.386*y)/g1^26 + 2*g1^14*t^8.638*y + (2*t^8.675*y)/g1^4 + g1^18*t^8.963*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
46931 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$ 0.7185 0.9121 0.7877 [M:[0.6738, 1.1087, 0.7826, 0.8913, 0.6738], q:[0.7772, 0.549], qb:[0.451, 0.4403], phi:[0.4456]] 2*t^2.022 + t^2.348 + 2*t^2.674 + t^2.968 + t^3. + t^3.685 + t^4.011 + 4*t^4.043 + t^4.305 + t^4.337 + 2*t^4.369 + t^4.631 + 5*t^4.695 + 2*t^4.989 + 4*t^5.022 + t^5.315 + 4*t^5.348 + 2*t^5.642 + t^5.674 + t^5.706 + t^5.935 - 2*t^6. - t^4.337/y - t^4.337*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
46181 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ 0.688 0.8542 0.8054 [M:[0.6814, 1.1062, 0.7876], q:[0.7766, 0.5421], qb:[0.4579, 0.4359], phi:[0.4469]] t^2.044 + t^2.363 + t^2.681 + t^2.934 + t^3. + t^3.319 + t^3.703 + t^3.956 + t^4.022 + 2*t^4.088 + t^4.275 + t^4.341 + t^4.407 + t^4.593 + 2*t^4.725 + t^4.978 + 2*t^5.044 + t^5.297 + 3*t^5.363 + t^5.615 + t^5.681 + t^5.868 - t^4.341/y - t^4.341*y detail