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
57422 SU3adj1nf2 ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ 1.495 1.7254 0.8665 [M:[0.6716], q:[0.5, 0.4926], qb:[0.5, 0.4926], phi:[0.3358]] [M:[[2, -2]], q:[[-3, 0], [-6, 3]], qb:[[3, 0], [0, 3]], phi:[[1, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{5}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ 2}\phi_{1}^{3}q_{1}\tilde{q}_{2}$ 1 2*t^2.015 + t^2.956 + 2*t^2.978 + t^3. + t^3.022 + t^3.963 + t^3.985 + t^4.007 + 3*t^4.03 + 3*t^4.97 + 6*t^4.993 + 3*t^5.015 + 2*t^5.037 + 2*t^5.463 + 2*t^5.485 + t^5.911 + 2*t^5.934 + 4*t^5.956 + 3*t^5.978 + t^6. + t^6.022 + 5*t^6.044 + 2*t^6.47 + 2*t^6.493 + t^6.919 + 3*t^6.941 + 4*t^6.963 + 7*t^6.985 + 9*t^7.007 + 4*t^7.03 + 3*t^7.052 + 2*t^7.456 + 4*t^7.478 + 4*t^7.5 + 2*t^7.522 + 4*t^7.926 + 8*t^7.948 + 13*t^7.97 + 8*t^7.993 + 3*t^8.015 + 7*t^8.059 + 2*t^8.419 + 6*t^8.441 + 4*t^8.463 + 2*t^8.485 - 2*t^8.53 + t^8.867 + 2*t^8.889 + 4*t^8.911 + 8*t^8.934 + 6*t^8.956 + 3*t^8.978 - t^4.007/y - t^5.015/y - (2*t^6.022)/y - t^6.963/y - (2*t^6.985)/y - t^7.007/y - (2*t^7.03)/y + t^7.97/y + (4*t^7.993)/y + t^8.015/y - (2*t^8.037)/y + (2*t^8.934)/y + (2*t^8.956)/y + (2*t^8.978)/y - t^4.007*y - t^5.015*y - 2*t^6.022*y - t^6.963*y - 2*t^6.985*y - t^7.007*y - 2*t^7.03*y + t^7.97*y + 4*t^7.993*y + t^8.015*y - 2*t^8.037*y + 2*t^8.934*y + 2*t^8.956*y + 2*t^8.978*y (2*g1^2*t^2.015)/g2^2 + (g2^6*t^2.956)/g1^6 + (2*g2^3*t^2.978)/g1^3 + t^3. + (g1^3*t^3.022)/g2^3 + (g2^5*t^3.963)/g1^5 + (g2^2*t^3.985)/g1^2 + (g1*t^4.007)/g2 + (3*g1^4*t^4.03)/g2^4 + (3*g2^4*t^4.97)/g1^4 + (6*g2*t^4.993)/g1 + (3*g1^2*t^5.015)/g2^2 + (2*g1^5*t^5.037)/g2^5 + (g2^5*t^5.463)/g1^14 + g1^4*g2^5*t^5.463 + (g2^2*t^5.485)/g1^11 + g1^7*g2^2*t^5.485 + (g2^12*t^5.911)/g1^12 + (2*g2^9*t^5.934)/g1^9 + (4*g2^6*t^5.956)/g1^6 + (3*g2^3*t^5.978)/g1^3 + t^6. + (g1^3*t^6.022)/g2^3 + (5*g1^6*t^6.044)/g2^6 + (g2^4*t^6.47)/g1^13 + g1^5*g2^4*t^6.47 + (g2*t^6.493)/g1^10 + g1^8*g2*t^6.493 + (g2^11*t^6.919)/g1^11 + (3*g2^8*t^6.941)/g1^8 + (4*g2^5*t^6.963)/g1^5 + (7*g2^2*t^6.985)/g1^2 + (9*g1*t^7.007)/g2 + (4*g1^4*t^7.03)/g2^4 + (3*g1^7*t^7.052)/g2^7 + (g2^6*t^7.456)/g1^15 + g1^3*g2^6*t^7.456 + (2*g2^3*t^7.478)/g1^12 + 2*g1^6*g2^3*t^7.478 + (2*t^7.5)/g1^9 + 2*g1^9*t^7.5 + t^7.522/(g1^6*g2^3) + (g1^12*t^7.522)/g2^3 + (4*g2^10*t^7.926)/g1^10 + (8*g2^7*t^7.948)/g1^7 + (13*g2^4*t^7.97)/g1^4 + (8*g2*t^7.993)/g1 + (3*g1^2*t^8.015)/g2^2 + (7*g1^8*t^8.059)/g2^8 + (g2^11*t^8.419)/g1^20 + (g2^11*t^8.419)/g1^2 + (3*g2^8*t^8.441)/g1^17 + 3*g1*g2^8*t^8.441 + (2*g2^5*t^8.463)/g1^14 + 2*g1^4*g2^5*t^8.463 + (g2^2*t^8.485)/g1^11 + g1^7*g2^2*t^8.485 - t^8.53/(g1^5*g2^4) - (g1^13*t^8.53)/g2^4 + (g2^18*t^8.867)/g1^18 + (2*g2^15*t^8.889)/g1^15 + (4*g2^12*t^8.911)/g1^12 + (8*g2^9*t^8.934)/g1^9 + (6*g2^6*t^8.956)/g1^6 + (3*g2^3*t^8.978)/g1^3 - (g1*t^4.007)/(g2*y) - (g1^2*t^5.015)/(g2^2*y) - (2*g1^3*t^6.022)/(g2^3*y) - (g2^5*t^6.963)/(g1^5*y) - (2*g2^2*t^6.985)/(g1^2*y) - (g1*t^7.007)/(g2*y) - (2*g1^4*t^7.03)/(g2^4*y) + (g2^4*t^7.97)/(g1^4*y) + (4*g2*t^7.993)/(g1*y) + (g1^2*t^8.015)/(g2^2*y) - (2*g1^5*t^8.037)/(g2^5*y) + (2*g2^9*t^8.934)/(g1^9*y) + (2*g2^6*t^8.956)/(g1^6*y) + (2*g2^3*t^8.978)/(g1^3*y) - (g1*t^4.007*y)/g2 - (g1^2*t^5.015*y)/g2^2 - (2*g1^3*t^6.022*y)/g2^3 - (g2^5*t^6.963*y)/g1^5 - (2*g2^2*t^6.985*y)/g1^2 - (g1*t^7.007*y)/g2 - (2*g1^4*t^7.03*y)/g2^4 + (g2^4*t^7.97*y)/g1^4 + (4*g2*t^7.993*y)/g1 + (g1^2*t^8.015*y)/g2^2 - (2*g1^5*t^8.037*y)/g2^5 + (2*g2^9*t^8.934*y)/g1^9 + (2*g2^6*t^8.956*y)/g1^6 + (2*g2^3*t^8.978*y)/g1^3


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
60207 ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{3}$ 1.4963 1.7305 0.8647 [X:[], M:[0.6812, 0.9781], q:[0.5, 0.4781], qb:[0.5, 0.4781], phi:[0.3406]] 2*t^2.04 + t^2.87 + 3*t^2.93 + t^3. + t^3.89 + t^3.96 + t^4.02 + 3*t^4.09 + 3*t^4.91 + 8*t^4.98 + 3*t^5.04 + 2*t^5.39 + 2*t^5.46 + t^5.74 + 3*t^5.8 + 7*t^5.87 + 3*t^5.93 - t^6. - t^4.02/y - t^5.04/y - t^4.02*y - t^5.04*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
47900 SU3adj1nf2 ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ 1.495 1.7254 0.8664 [M:[0.6707], q:[0.4996, 0.493], qb:[0.5004, 0.4921], phi:[0.3358]] t^2.012 + t^2.015 + t^2.955 + t^2.975 + t^2.98 + t^3. + t^3.022 + t^3.963 + t^3.982 + t^4.007 + t^4.024 + t^4.027 + t^4.03 + t^4.968 + 2*t^4.97 + t^4.987 + 2*t^4.99 + t^4.993 + 2*t^4.995 + t^5.012 + 2*t^5.015 + t^5.035 + t^5.037 + t^5.462 + t^5.464 + t^5.484 + t^5.486 + t^5.911 + t^5.93 + t^5.936 + t^5.95 + 2*t^5.955 + t^5.961 + t^5.975 + 2*t^5.978 + t^5.995 + 2*t^5.997 - 3*t^6. - t^4.007/y - t^5.015/y - t^4.007*y - t^5.015*y detail