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
58378 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }M_{2}\phi_{1}^{3}$ 1.3633 1.6144 0.8444 [X:[1.4], M:[0.7819, 0.8], q:[0.3076, 0.4894], qb:[0.5106, 0.2924], phi:[0.4]] [X:[[0, 0]], M:[[-1, 1], [0, 0]], q:[[0, -1], [-1, 0]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ ${2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$ 0 2*t^2.35 + 2*t^2.4 + t^2.45 + 2*t^3. + t^3.55 + 3*t^4.2 + t^4.49 + t^4.51 + 3*t^4.69 + 5*t^4.75 + 5*t^4.8 + 3*t^4.85 + t^4.91 + t^5.06 + t^5.14 + 3*t^5.35 + 5*t^5.4 + t^5.45 + t^5.69 + t^5.71 + 2*t^5.89 + 2*t^5.95 + t^6.23 + t^6.26 + t^6.34 + t^6.37 + 6*t^6.55 + 5*t^6.6 + t^6.65 + 2*t^6.83 + t^6.86 + 3*t^6.89 + 3*t^6.91 + t^6.97 + 4*t^7.04 + 9*t^7.09 + 10*t^7.15 + 13*t^7.2 + 6*t^7.25 + 3*t^7.31 + t^7.36 + 2*t^7.4 + 3*t^7.46 + 2*t^7.49 + t^7.51 + 3*t^7.54 + t^7.6 + 4*t^7.69 + 11*t^7.75 + 7*t^7.8 + 3*t^7.85 + t^7.91 + t^8. + 2*t^8.03 + 2*t^8.06 + t^8.09 + t^8.11 + t^8.2 + 3*t^8.24 + 5*t^8.29 + 6*t^8.4 - 3*t^8.45 + 2*t^8.58 + 2*t^8.6 + t^8.63 + t^8.66 + 4*t^8.69 + 3*t^8.71 + t^8.74 + t^8.77 + t^8.82 + 8*t^8.89 + 13*t^8.95 + t^8.97 - t^4.2/y - t^5.4/y - (2*t^6.55)/y - (2*t^6.6)/y - t^6.65/y - t^7.2/y + t^7.69/y + (2*t^7.75)/y + (2*t^7.8)/y + (2*t^7.85)/y + (4*t^8.35)/y + t^8.4/y + (2*t^8.45)/y - t^8.89/y - (3*t^8.95)/y - t^4.2*y - t^5.4*y - 2*t^6.55*y - 2*t^6.6*y - t^6.65*y - t^7.2*y + t^7.69*y + 2*t^7.75*y + 2*t^7.8*y + 2*t^7.85*y + 4*t^8.35*y + t^8.4*y + 2*t^8.45*y - t^8.89*y - 3*t^8.95*y (2*g2*t^2.35)/g1 + 2*t^2.4 + (g1*t^2.45)/g2 + 2*t^3. + (g2*t^3.55)/g1 + 3*t^4.2 + g1*g2^2*t^4.49 + t^4.51/(g1*g2^2) + (3*g2^2*t^4.69)/g1^2 + (5*g2*t^4.75)/g1 + 5*t^4.8 + (3*g1*t^4.85)/g2 + (g1^2*t^4.91)/g2^2 + t^5.06/(g1^2*g2) + g1^2*g2*t^5.14 + (3*g2*t^5.35)/g1 + 5*t^5.4 + (g1*t^5.45)/g2 + g1*g2^2*t^5.69 + t^5.71/(g1*g2^2) + (2*g2^2*t^5.89)/g1^2 + (2*g2*t^5.95)/g1 + g2^3*t^6.23 + t^6.26/(g1^2*g2) + g1^2*g2*t^6.34 + t^6.37/g2^3 + (6*g2*t^6.55)/g1 + 5*t^6.6 + (g1*t^6.65)/g2 + 2*g2^3*t^6.83 + t^6.86/(g1^2*g2) + 3*g1*g2^2*t^6.89 + (3*t^6.91)/(g1*g2^2) + t^6.97/g2^3 + (4*g2^3*t^7.04)/g1^3 + (9*g2^2*t^7.09)/g1^2 + (10*g2*t^7.15)/g1 + 13*t^7.2 + (6*g1*t^7.25)/g2 + (3*g1^2*t^7.31)/g2^2 + (g1^3*t^7.36)/g2^3 + (2*t^7.4)/g1^3 + (3*t^7.46)/(g1^2*g2) + 2*g1*g2^2*t^7.49 + t^7.51/(g1*g2^2) + 3*g1^2*g2*t^7.54 + g1^3*t^7.6 + (4*g2^2*t^7.69)/g1^2 + (11*g2*t^7.75)/g1 + 7*t^7.8 + (3*g1*t^7.85)/g2 + (g1^2*t^7.91)/g2^2 + t^8./g1^3 + 2*g2^3*t^8.03 + (2*t^8.06)/(g1^2*g2) + g1*g2^2*t^8.09 + t^8.11/(g1*g2^2) + g1^3*t^8.2 + (3*g2^3*t^8.24)/g1^3 + (5*g2^2*t^8.29)/g1^2 + 6*t^8.4 - (3*g1*t^8.45)/g2 + (2*g2^4*t^8.58)/g1 + (2*t^8.6)/g1^3 + g2^3*t^8.63 + t^8.66/(g1^2*g2) + 4*g1*g2^2*t^8.69 + (3*t^8.71)/(g1*g2^2) + g1^2*g2*t^8.74 + t^8.77/g2^3 + (g1*t^8.82)/g2^4 + (8*g2^2*t^8.89)/g1^2 + (13*g2*t^8.95)/g1 + g1^2*g2^4*t^8.97 - t^4.2/y - t^5.4/y - (2*g2*t^6.55)/(g1*y) - (2*t^6.6)/y - (g1*t^6.65)/(g2*y) - t^7.2/y + (g2^2*t^7.69)/(g1^2*y) + (2*g2*t^7.75)/(g1*y) + (2*t^7.8)/y + (2*g1*t^7.85)/(g2*y) + (4*g2*t^8.35)/(g1*y) + t^8.4/y + (2*g1*t^8.45)/(g2*y) - (g2^2*t^8.89)/(g1^2*y) - (3*g2*t^8.95)/(g1*y) - t^4.2*y - t^5.4*y - (2*g2*t^6.55*y)/g1 - 2*t^6.6*y - (g1*t^6.65*y)/g2 - t^7.2*y + (g2^2*t^7.69*y)/g1^2 + (2*g2*t^7.75*y)/g1 + 2*t^7.8*y + (2*g1*t^7.85*y)/g2 + (4*g2*t^8.35*y)/g1 + t^8.4*y + (2*g1*t^8.45*y)/g2 - (g2^2*t^8.89*y)/g1^2 - (3*g2*t^8.95*y)/g1


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
57346 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ 1.3468 1.5854 0.8495 [X:[1.4], M:[0.7819], q:[0.3076, 0.4894], qb:[0.5106, 0.2924], phi:[0.4]] 2*t^2.346 + t^2.4 + t^2.454 + 2*t^3. + t^3.546 + t^3.6 + 3*t^4.2 + t^4.486 + t^4.514 + 3*t^4.691 + 3*t^4.746 + 3*t^4.8 + 2*t^4.854 + t^4.909 + t^5.059 + t^5.141 + 3*t^5.346 + 3*t^5.4 + t^5.454 + t^5.686 + t^5.714 + 2*t^5.891 + 3*t^5.946 + t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail