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
45898 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ 0.6965 0.8595 0.8103 [M:[0.9459, 0.9459], q:[0.5541, 0.5], qb:[0.5, 0.4459], phi:[0.5]] [M:[[1, 1], [-1, 1]], q:[[0, -1], [-1, 0]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ -1 4*t^2.838 + 3*t^3. + t^4.175 + 2*t^4.338 + 4*t^4.5 + 2*t^4.662 + t^4.825 + 9*t^5.675 + 8*t^5.838 - t^6. - 4*t^6.162 - t^6.325 + 4*t^7.013 + 8*t^7.175 + 12*t^7.338 + 6*t^7.5 + t^8.351 + 18*t^8.513 + 17*t^8.675 - 6*t^8.838 - t^4.5/y - (2*t^7.338)/y + (2*t^7.662)/y + (6*t^8.675)/y + (12*t^8.838)/y - t^4.5*y - 2*t^7.338*y + 2*t^7.662*y + 6*t^8.675*y + 12*t^8.838*y (2*g2*t^2.838)/g1 + 2*g1*g2*t^2.838 + 3*t^3. + g2^2*t^4.175 + (g2*t^4.338)/g1 + g1*g2*t^4.338 + 2*t^4.5 + t^4.5/g1^2 + g1^2*t^4.5 + t^4.662/(g1*g2) + (g1*t^4.662)/g2 + t^4.825/g2^2 + 3*g2^2*t^5.675 + (3*g2^2*t^5.675)/g1^2 + 3*g1^2*g2^2*t^5.675 + (4*g2*t^5.838)/g1 + 4*g1*g2*t^5.838 + t^6. - t^6./g1^2 - g1^2*t^6. - (2*t^6.162)/(g1*g2) - (2*g1*t^6.162)/g2 - t^6.325/g2^2 + (2*g2^3*t^7.013)/g1 + 2*g1*g2^3*t^7.013 + 4*g2^2*t^7.175 + (2*g2^2*t^7.175)/g1^2 + 2*g1^2*g2^2*t^7.175 + (2*g2*t^7.338)/g1^3 + (4*g2*t^7.338)/g1 + 4*g1*g2*t^7.338 + 2*g1^3*g2*t^7.338 + 2*t^7.5 + (2*t^7.5)/g1^2 + 2*g1^2*t^7.5 + g2^4*t^8.351 + (4*g2^3*t^8.513)/g1^3 + (5*g2^3*t^8.513)/g1 + 5*g1*g2^3*t^8.513 + 4*g1^3*g2^3*t^8.513 + 5*g2^2*t^8.675 + (6*g2^2*t^8.675)/g1^2 + 6*g1^2*g2^2*t^8.675 - (g2*t^8.838)/g1^3 - (2*g2*t^8.838)/g1 - 2*g1*g2*t^8.838 - g1^3*g2*t^8.838 - t^4.5/y - (g2*t^7.338)/(g1*y) - (g1*g2*t^7.338)/y + t^7.662/(g1*g2*y) + (g1*t^7.662)/(g2*y) + (4*g2^2*t^8.675)/y + (g2^2*t^8.675)/(g1^2*y) + (g1^2*g2^2*t^8.675)/y + (6*g2*t^8.838)/(g1*y) + (6*g1*g2*t^8.838)/y - t^4.5*y - (g2*t^7.338*y)/g1 - g1*g2*t^7.338*y + (t^7.662*y)/(g1*g2) + (g1*t^7.662*y)/g2 + 4*g2^2*t^8.675*y + (g2^2*t^8.675*y)/g1^2 + g1^2*g2^2*t^8.675*y + (6*g2*t^8.838*y)/g1 + 6*g1*g2*t^8.838*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
45862 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ 0.6965 0.8596 0.8103 [M:[0.9458, 0.9458], q:[0.5557, 0.4985], qb:[0.4985, 0.4472], phi:[0.5]] 4*t^2.837 + t^2.991 + t^3. + t^3.009 + t^4.183 + 2*t^4.337 + 3*t^4.491 + t^4.509 + 2*t^4.663 + t^4.834 + 9*t^5.675 + 2*t^5.828 + 4*t^5.837 + 2*t^5.846 + t^5.982 + t^5.991 - 5*t^6. - t^4.5/y - t^4.5*y detail