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
2506 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{1}M_{7}$ 0.7086 0.875 0.8098 [M:[1.0361, 0.8918, 1.0721, 0.8558, 1.0, 0.9279, 0.9639], q:[0.4459, 0.518], qb:[0.482, 0.6262], phi:[0.482]] [M:[[2], [-6], [4], [-8], [0], [-4], [-2]], q:[[-3], [1]], qb:[[-1], [7]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{3}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{3}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$ ${}$ -2 t^2.567 + t^2.675 + t^2.784 + 2*t^2.892 + t^3. + t^3.216 + t^4.121 + t^4.23 + 2*t^4.338 + t^4.446 + t^4.554 + t^4.662 + t^4.77 + t^4.879 + t^5.135 + t^5.203 + t^5.243 + 2*t^5.351 + 2*t^5.459 + 3*t^5.567 + 2*t^5.675 + 4*t^5.784 + t^5.892 - 2*t^6. - t^6.216 - t^6.325 - t^6.541 + t^6.689 + 2*t^6.797 + 3*t^6.905 + 5*t^7.013 + 5*t^7.121 + 5*t^7.23 + 4*t^7.338 + t^7.446 + 2*t^7.554 + t^7.702 + t^7.77 + t^7.81 + 2*t^7.918 - t^7.987 + 3*t^8.026 + 2*t^8.095 + 3*t^8.135 + 5*t^8.243 - t^8.311 + 5*t^8.351 + t^8.42 + 5*t^8.459 + 2*t^8.567 + 2*t^8.675 - t^8.784 - 6*t^8.892 - t^4.446/y - t^7.013/y - t^7.121/y - t^7.338/y + t^7.554/y + t^7.77/y + t^7.879/y + t^8.243/y + t^8.351/y + (3*t^8.459)/y + (3*t^8.567)/y + (3*t^8.675)/y + (3*t^8.784)/y + (3*t^8.892)/y - t^4.446*y - t^7.013*y - t^7.121*y - t^7.338*y + t^7.554*y + t^7.77*y + t^7.879*y + t^8.243*y + t^8.351*y + 3*t^8.459*y + 3*t^8.567*y + 3*t^8.675*y + 3*t^8.784*y + 3*t^8.892*y t^2.567/g1^8 + t^2.675/g1^6 + t^2.784/g1^4 + (2*t^2.892)/g1^2 + t^3. + g1^4*t^3.216 + t^4.121/g1^7 + t^4.23/g1^5 + (2*t^4.338)/g1^3 + t^4.446/g1 + g1*t^4.554 + g1^3*t^4.662 + g1^5*t^4.77 + g1^7*t^4.879 + t^5.135/g1^16 + g1^13*t^5.203 + t^5.243/g1^14 + (2*t^5.351)/g1^12 + (2*t^5.459)/g1^10 + (3*t^5.567)/g1^8 + (2*t^5.675)/g1^6 + (4*t^5.784)/g1^4 + t^5.892/g1^2 - 2*t^6. - g1^4*t^6.216 - g1^6*t^6.325 - g1^10*t^6.541 + t^6.689/g1^15 + (2*t^6.797)/g1^13 + (3*t^6.905)/g1^11 + (5*t^7.013)/g1^9 + (5*t^7.121)/g1^7 + (5*t^7.23)/g1^5 + (4*t^7.338)/g1^3 + t^7.446/g1 + 2*g1*t^7.554 + t^7.702/g1^24 + g1^5*t^7.77 + t^7.81/g1^22 + (2*t^7.918)/g1^20 - g1^9*t^7.987 + (3*t^8.026)/g1^18 + 2*g1^11*t^8.095 + (3*t^8.135)/g1^16 + (5*t^8.243)/g1^14 - g1^15*t^8.311 + (5*t^8.351)/g1^12 + g1^17*t^8.42 + (5*t^8.459)/g1^10 + (2*t^8.567)/g1^8 + (2*t^8.675)/g1^6 - t^8.784/g1^4 - (6*t^8.892)/g1^2 - t^4.446/(g1*y) - t^7.013/(g1^9*y) - t^7.121/(g1^7*y) - t^7.338/(g1^3*y) + (g1*t^7.554)/y + (g1^5*t^7.77)/y + (g1^7*t^7.879)/y + t^8.243/(g1^14*y) + t^8.351/(g1^12*y) + (3*t^8.459)/(g1^10*y) + (3*t^8.567)/(g1^8*y) + (3*t^8.675)/(g1^6*y) + (3*t^8.784)/(g1^4*y) + (3*t^8.892)/(g1^2*y) - (t^4.446*y)/g1 - (t^7.013*y)/g1^9 - (t^7.121*y)/g1^7 - (t^7.338*y)/g1^3 + g1*t^7.554*y + g1^5*t^7.77*y + g1^7*t^7.879*y + (t^8.243*y)/g1^14 + (t^8.351*y)/g1^12 + (3*t^8.459*y)/g1^10 + (3*t^8.567*y)/g1^8 + (3*t^8.675*y)/g1^6 + (3*t^8.784*y)/g1^4 + (3*t^8.892*y)/g1^2


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
1434 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{6}$ 0.7054 0.8688 0.8119 [M:[1.0326, 0.9023, 1.0652, 0.8697, 1.0, 0.9348], q:[0.4511, 0.5163], qb:[0.4837, 0.614], phi:[0.4837]] t^2.609 + t^2.707 + t^2.805 + t^2.902 + t^3. + t^3.098 + t^3.195 + t^4.158 + t^4.256 + 2*t^4.353 + t^4.451 + t^4.549 + t^4.647 + t^4.744 + t^4.842 + t^5.135 + t^5.218 + t^5.316 + 2*t^5.414 + t^5.511 + 2*t^5.609 + 2*t^5.707 + 3*t^5.805 + t^5.902 - t^6. - t^4.451/y - t^4.451*y detail