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
581 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ 0.6975 0.8554 0.8154 [M:[0.9459, 1.018, 1.0541, 0.9098], q:[0.491, 0.5631], qb:[0.4549, 0.5271], phi:[0.491]] [M:[[-6], [2], [6], [-10]], q:[[-1], [7]], qb:[[-5], [3]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}^{4}$ ${}\phi_{1}^{2}q_{2}\tilde{q}_{1}$ 0 t^2.729 + t^2.838 + t^2.946 + 3*t^3.054 + t^3.162 + t^4.202 + t^4.311 + 2*t^4.419 + 2*t^4.527 + 2*t^4.635 + t^4.743 + t^4.852 + t^5.459 + t^5.567 + t^5.675 + 2*t^5.784 + 2*t^5.892 + 3*t^6.108 + t^6.216 + t^6.932 + 2*t^7.04 + 3*t^7.148 + 4*t^7.257 + 4*t^7.365 + 4*t^7.473 + 4*t^7.581 + 3*t^7.689 + 2*t^7.798 + 2*t^7.906 + t^8.014 + t^8.188 + t^8.297 + 2*t^8.405 + 3*t^8.513 + 3*t^8.621 + t^8.729 + t^8.838 - t^4.473/y - t^7.202/y + t^7.743/y + t^8.567/y + t^8.675/y + (4*t^8.784)/y + (4*t^8.892)/y - t^4.473*y - t^7.202*y + t^7.743*y + t^8.567*y + t^8.675*y + 4*t^8.784*y + 4*t^8.892*y t^2.729/g1^10 + t^2.838/g1^6 + t^2.946/g1^2 + 3*g1^2*t^3.054 + g1^6*t^3.162 + t^4.202/g1^11 + t^4.311/g1^7 + (2*t^4.419)/g1^3 + 2*g1*t^4.527 + 2*g1^5*t^4.635 + g1^9*t^4.743 + g1^13*t^4.852 + t^5.459/g1^20 + t^5.567/g1^16 + t^5.675/g1^12 + (2*t^5.784)/g1^8 + (2*t^5.892)/g1^4 + 3*g1^4*t^6.108 + g1^8*t^6.216 + t^6.932/g1^21 + (2*t^7.04)/g1^17 + (3*t^7.148)/g1^13 + (4*t^7.257)/g1^9 + (4*t^7.365)/g1^5 + (4*t^7.473)/g1 + 4*g1^3*t^7.581 + 3*g1^7*t^7.689 + 2*g1^11*t^7.798 + 2*g1^15*t^7.906 + g1^19*t^8.014 + t^8.188/g1^30 + t^8.297/g1^26 + (2*t^8.405)/g1^22 + (3*t^8.513)/g1^18 + (3*t^8.621)/g1^14 + t^8.729/g1^10 + t^8.838/g1^6 - t^4.473/(g1*y) - t^7.202/(g1^11*y) + (g1^9*t^7.743)/y + t^8.567/(g1^16*y) + t^8.675/(g1^12*y) + (4*t^8.784)/(g1^8*y) + (4*t^8.892)/(g1^4*y) - (t^4.473*y)/g1 - (t^7.202*y)/g1^11 + g1^9*t^7.743*y + (t^8.567*y)/g1^16 + (t^8.675*y)/g1^12 + (4*t^8.784*y)/g1^8 + (4*t^8.892*y)/g1^4


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
904 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}^{2}$ 0.6959 0.8526 0.8162 [M:[0.9533, 1.0156, 1.0467, 0.9222, 1.0156], q:[0.4922, 0.5545], qb:[0.4611, 0.5233], phi:[0.4922]] t^2.767 + t^2.86 + 4*t^3.047 + t^3.14 + t^4.243 + t^4.337 + 2*t^4.43 + 2*t^4.523 + 2*t^4.617 + t^4.71 + t^4.804 + t^5.533 + t^5.626 + 2*t^5.813 + 2*t^5.907 - 3*t^6. - t^4.477/y - t^4.477*y detail
1922 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{4}X_{1}$ 0.6079 0.7473 0.8134 [X:[1.3846], M:[0.7692, 1.0769, 1.2308, 0.6154], q:[0.4615, 0.7692], qb:[0.3077, 0.6154], phi:[0.4615]] t^2.308 + t^2.769 + 4*t^3.231 + 2*t^3.692 + 3*t^4.154 + 2*t^4.615 + t^5.077 + 3*t^5.538 + 2*t^6. - t^4.385/y - t^4.385*y detail {a: 21369/35152, c: 13135/17576, X1: 18/13, M1: 10/13, M2: 14/13, M3: 16/13, M4: 8/13, q1: 6/13, q2: 10/13, qb1: 4/13, qb2: 8/13, phi1: 6/13}


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
366 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ 0.6975 0.8554 0.8154 [M:[0.9458, 1.0181, 1.0542, 0.9096], q:[0.4896, 0.5646], qb:[0.4562, 0.5258], phi:[0.491]] t^2.729 + t^2.837 + t^2.946 + t^3.046 + t^3.054 + t^3.062 + t^3.163 + t^4.21 + t^4.31 + t^4.411 + t^4.419 + t^4.519 + t^4.535 + t^4.628 + t^4.636 + t^4.744 + t^4.86 + t^5.458 + t^5.566 + t^5.675 + 2*t^5.783 + 2*t^5.892 + t^5.992 - 2*t^6. - t^4.473/y - t^4.473*y detail