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
815 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ 0.6127 0.7931 0.7725 [M:[1.0, 1.1136, 0.7728, 0.7728, 0.6704], q:[0.7784, 0.2216], qb:[0.5623, 0.6648], phi:[0.4432]] [M:[[0], [-4], [8], [8], [-6]], q:[[-1], [1]], qb:[[-11], [3]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }M_{3}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }M_{5}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}^{2}q_{2}^{4}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ ${}$ -2 t^2.011 + 2*t^2.319 + t^2.352 + 2*t^2.659 + t^3. + t^3.341 + 2*t^4.022 + 3*t^4.33 + t^4.363 + 3*t^4.637 + 3*t^4.67 + 2*t^4.704 + 3*t^4.978 + 4*t^5.011 + 6*t^5.319 + 2*t^5.352 + 3*t^5.659 - 2*t^6. + 2*t^6.033 - 2*t^6.307 + 4*t^6.341 + 2*t^6.374 + 4*t^6.648 + 4*t^6.681 + 2*t^6.715 + 4*t^6.956 + 4*t^6.989 + 5*t^7.022 + 2*t^7.055 + 4*t^7.296 + 6*t^7.33 + 6*t^7.363 + 8*t^7.637 + 7*t^7.67 + t^7.704 + 9*t^7.978 - 2*t^8.011 + 3*t^8.044 - 5*t^8.319 + t^8.352 + 2*t^8.385 - 3*t^8.626 - t^8.659 + 2*t^8.693 + 4*t^8.726 + 2*t^8.967 - t^4.33/y - t^6.341/y - (2*t^6.648)/y + (2*t^7.33)/y + t^7.363/y + t^7.637/y + (4*t^7.67)/y + (4*t^7.978)/y + (5*t^8.011)/y + (4*t^8.319)/y + t^8.352/y + (2*t^8.659)/y + t^8.693/y - (3*t^8.967)/y - t^4.33*y - t^6.341*y - 2*t^6.648*y + 2*t^7.33*y + t^7.363*y + t^7.637*y + 4*t^7.67*y + 4*t^7.978*y + 5*t^8.011*y + 4*t^8.319*y + t^8.352*y + 2*t^8.659*y + t^8.693*y - 3*t^8.967*y t^2.011/g1^6 + 2*g1^8*t^2.319 + t^2.352/g1^10 + 2*g1^4*t^2.659 + t^3. + t^3.341/g1^4 + (2*t^4.022)/g1^12 + 3*g1^2*t^4.33 + t^4.363/g1^16 + 3*g1^16*t^4.637 + (3*t^4.67)/g1^2 + (2*t^4.704)/g1^20 + 3*g1^12*t^4.978 + (4*t^5.011)/g1^6 + 6*g1^8*t^5.319 + (2*t^5.352)/g1^10 + 3*g1^4*t^5.659 - 2*t^6. + (2*t^6.033)/g1^18 - 2*g1^14*t^6.307 + (4*t^6.341)/g1^4 + (2*t^6.374)/g1^22 + 4*g1^10*t^6.648 + (4*t^6.681)/g1^8 + (2*t^6.715)/g1^26 + 4*g1^24*t^6.956 + 4*g1^6*t^6.989 + (5*t^7.022)/g1^12 + (2*t^7.055)/g1^30 + 4*g1^20*t^7.296 + 6*g1^2*t^7.33 + (6*t^7.363)/g1^16 + 8*g1^16*t^7.637 + (7*t^7.67)/g1^2 + t^7.704/g1^20 + 9*g1^12*t^7.978 - (2*t^8.011)/g1^6 + (3*t^8.044)/g1^24 - 5*g1^8*t^8.319 + t^8.352/g1^10 + (2*t^8.385)/g1^28 - 3*g1^22*t^8.626 - g1^4*t^8.659 + (2*t^8.693)/g1^14 + (4*t^8.726)/g1^32 + 2*g1^18*t^8.967 - (g1^2*t^4.33)/y - t^6.341/(g1^4*y) - (2*g1^10*t^6.648)/y + (2*g1^2*t^7.33)/y + t^7.363/(g1^16*y) + (g1^16*t^7.637)/y + (4*t^7.67)/(g1^2*y) + (4*g1^12*t^7.978)/y + (5*t^8.011)/(g1^6*y) + (4*g1^8*t^8.319)/y + t^8.352/(g1^10*y) + (2*g1^4*t^8.659)/y + t^8.693/(g1^14*y) - (3*g1^18*t^8.967)/y - g1^2*t^4.33*y - (t^6.341*y)/g1^4 - 2*g1^10*t^6.648*y + 2*g1^2*t^7.33*y + (t^7.363*y)/g1^16 + g1^16*t^7.637*y + (4*t^7.67*y)/g1^2 + 4*g1^12*t^7.978*y + (5*t^8.011*y)/g1^6 + 4*g1^8*t^8.319*y + (t^8.352*y)/g1^10 + 2*g1^4*t^8.659*y + (t^8.693*y)/g1^14 - 3*g1^18*t^8.967*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
522 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ 0.5919 0.7517 0.7874 [M:[1.0, 1.1138, 0.7725, 0.7725], q:[0.7784, 0.2216], qb:[0.5629, 0.6647], phi:[0.4431]] 2*t^2.317 + t^2.353 + 2*t^2.659 + t^3. + t^3.341 + t^3.988 + t^4.024 + t^4.329 + 3*t^4.635 + t^4.671 + 2*t^4.707 + 3*t^4.976 + 3*t^5.012 + 6*t^5.317 + t^5.353 + 3*t^5.659 - 2*t^6. - t^4.329/y - t^4.329*y detail