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
2767 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}q_{1}q_{2}$ + ${ }M_{5}q_{1}q_{2}$ 0.6543 0.8436 0.7756 [M:[1.1103, 1.1397, 0.75, 0.7206, 0.75], q:[0.75, 0.5], qb:[0.3897, 0.3603], phi:[0.5]] [M:[[1], [-1], [0], [2], [0]], q:[[0], [0]], qb:[[-1], [1]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{3}$, ${ }M_{5}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{5}q_{1}\tilde{q}_{1}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ ${}$ -3 t^2.162 + 3*t^2.25 + t^3. + 2*t^3.331 + 2*t^3.419 + t^3.662 + t^4.081 + t^4.169 + t^4.324 + 3*t^4.412 + 7*t^4.5 + t^5.162 + 3*t^5.25 + 2*t^5.493 + 7*t^5.581 + 5*t^5.669 + t^5.824 + 2*t^5.912 - 3*t^6. - t^6.088 + t^6.243 + 3*t^6.331 + 2*t^6.419 + t^6.486 + 3*t^6.574 + 10*t^6.662 + 13*t^6.75 + 2*t^6.838 + 2*t^6.993 - t^7.081 - 3*t^7.169 + 2*t^7.324 + 3*t^7.412 + 5*t^7.5 + 2*t^7.655 + 8*t^7.743 + 13*t^7.831 + 7*t^7.919 + t^7.986 + 2*t^8.074 + t^8.162 - 11*t^8.25 - 3*t^8.338 + t^8.405 + 3*t^8.493 + 5*t^8.581 + t^8.647 + 3*t^8.669 + 3*t^8.736 + 10*t^8.824 + 19*t^8.912 - t^4.5/y - t^6.662/y - (2*t^6.75)/y + t^7.081/y + t^7.169/y + (3*t^7.412)/y + (3*t^7.5)/y - t^7.831/y - t^7.919/y + t^8.162/y + (5*t^8.25)/y + t^8.338/y + (2*t^8.493)/y + (8*t^8.581)/y + (6*t^8.669)/y + t^8.912/y - t^4.5*y - t^6.662*y - 2*t^6.75*y + t^7.081*y + t^7.169*y + 3*t^7.412*y + 3*t^7.5*y - t^7.831*y - t^7.919*y + t^8.162*y + 5*t^8.25*y + t^8.338*y + 2*t^8.493*y + 8*t^8.581*y + 6*t^8.669*y + t^8.912*y g1^2*t^2.162 + 3*t^2.25 + t^3. + 2*g1*t^3.331 + (2*t^3.419)/g1 + g1^2*t^3.662 + g1*t^4.081 + t^4.169/g1 + g1^4*t^4.324 + 3*g1^2*t^4.412 + 7*t^4.5 + g1^2*t^5.162 + 3*t^5.25 + 2*g1^3*t^5.493 + 7*g1*t^5.581 + (5*t^5.669)/g1 + g1^4*t^5.824 + 2*g1^2*t^5.912 - 3*t^6. - t^6.088/g1^2 + g1^3*t^6.243 + 3*g1*t^6.331 + (2*t^6.419)/g1 + g1^6*t^6.486 + 3*g1^4*t^6.574 + 10*g1^2*t^6.662 + 13*t^6.75 + (2*t^6.838)/g1^2 + 2*g1^3*t^6.993 - g1*t^7.081 - (3*t^7.169)/g1 + 2*g1^4*t^7.324 + 3*g1^2*t^7.412 + 5*t^7.5 + 2*g1^5*t^7.655 + 8*g1^3*t^7.743 + 13*g1*t^7.831 + (7*t^7.919)/g1 + g1^6*t^7.986 + 2*g1^4*t^8.074 + g1^2*t^8.162 - 11*t^8.25 - (3*t^8.338)/g1^2 + g1^5*t^8.405 + 3*g1^3*t^8.493 + 5*g1*t^8.581 + g1^8*t^8.647 + (3*t^8.669)/g1 + 3*g1^6*t^8.736 + 10*g1^4*t^8.824 + 19*g1^2*t^8.912 - t^4.5/y - (g1^2*t^6.662)/y - (2*t^6.75)/y + (g1*t^7.081)/y + t^7.169/(g1*y) + (3*g1^2*t^7.412)/y + (3*t^7.5)/y - (g1*t^7.831)/y - t^7.919/(g1*y) + (g1^2*t^8.162)/y + (5*t^8.25)/y + t^8.338/(g1^2*y) + (2*g1^3*t^8.493)/y + (8*g1*t^8.581)/y + (6*t^8.669)/(g1*y) + (g1^2*t^8.912)/y - t^4.5*y - g1^2*t^6.662*y - 2*t^6.75*y + g1*t^7.081*y + (t^7.169*y)/g1 + 3*g1^2*t^7.412*y + 3*t^7.5*y - g1*t^7.831*y - (t^7.919*y)/g1 + g1^2*t^8.162*y + 5*t^8.25*y + (t^8.338*y)/g1^2 + 2*g1^3*t^8.493*y + 8*g1*t^8.581*y + (6*t^8.669*y)/g1 + g1^2*t^8.912*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


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
1761 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}q_{1}q_{2}$ 0.6352 0.809 0.7853 [M:[1.1103, 1.1397, 0.75, 0.7206], q:[0.75, 0.5], qb:[0.3897, 0.3603], phi:[0.5]] t^2.162 + 2*t^2.25 + t^3. + 2*t^3.331 + 2*t^3.419 + t^3.662 + t^3.75 + t^4.081 + t^4.169 + t^4.324 + 2*t^4.412 + 4*t^4.5 + t^5.162 + 2*t^5.25 + 2*t^5.493 + 5*t^5.581 + 3*t^5.669 + t^5.824 + 2*t^5.912 - t^6. - t^4.5/y - t^4.5*y detail