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
46574 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{5}$ 0.6058 0.7557 0.8017 [M:[1.0133, 0.9867, 0.742, 0.7954, 0.9867], q:[0.5765, 0.4101], qb:[0.4368, 1.0391], phi:[0.3844]] [M:[[1, -3], [-1, 3], [-2, 2], [2, -10], [-1, 3]], q:[[0, -3], [-1, 6]], qb:[[1, 0], [0, 5]], phi:[[0, -2]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}^{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$ -2 t^2.226 + t^2.306 + t^2.386 + t^2.541 + 2*t^2.96 + t^3.694 + t^4.348 + t^4.428 + t^4.452 + t^4.532 + 2*t^4.612 + t^4.692 + t^4.767 + t^4.772 + 2*t^4.847 + t^4.927 + t^5.082 + 2*t^5.186 + t^5.266 + t^5.346 + 2*t^5.501 + 3*t^5.92 - 2*t^6. + t^6.235 - t^6.419 - t^6.499 + t^6.574 + 2*t^6.654 + t^6.678 + t^6.758 + t^6.814 + 2*t^6.838 + t^6.889 + 2*t^6.918 + t^6.969 + t^6.993 + 2*t^6.998 + t^7.073 + t^7.078 + t^7.153 + t^7.159 + t^7.233 + 2*t^7.308 + t^7.313 + 2*t^7.388 + 2*t^7.412 + t^7.492 + 2*t^7.572 + t^7.623 + 2*t^7.727 + t^7.732 + t^7.807 - t^7.887 + 2*t^8.042 + 3*t^8.146 - 2*t^8.226 - t^8.306 - 3*t^8.386 + 2*t^8.461 - 3*t^8.541 - t^8.621 - t^8.645 + t^8.696 - t^8.725 + 2*t^8.776 + t^8.8 - t^8.805 + t^8.856 + 4*t^8.88 - t^8.885 + t^8.904 - 5*t^8.96 + t^8.984 - t^4.153/y - t^6.379/y - t^6.459/y - t^6.539/y - t^7.113/y + t^7.193/y + t^7.532/y + t^7.612/y + t^7.692/y + (2*t^7.767)/y + (2*t^7.847)/y + (2*t^7.927)/y + (2*t^8.186)/y + (2*t^8.266)/y + (2*t^8.346)/y + (2*t^8.501)/y - t^8.605/y - t^8.685/y - (2*t^8.765)/y - t^8.845/y + (2*t^8.92)/y - t^8.925/y - t^4.153*y - t^6.379*y - t^6.459*y - t^6.539*y - t^7.113*y + t^7.193*y + t^7.532*y + t^7.612*y + t^7.692*y + 2*t^7.767*y + 2*t^7.847*y + 2*t^7.927*y + 2*t^8.186*y + 2*t^8.266*y + 2*t^8.346*y + 2*t^8.501*y - t^8.605*y - t^8.685*y - 2*t^8.765*y - t^8.845*y + 2*t^8.92*y - t^8.925*y (g2^2*t^2.226)/g1^2 + t^2.306/g2^4 + (g1^2*t^2.386)/g2^10 + g2^6*t^2.541 + (2*g2^3*t^2.96)/g1 + g2^4*t^3.694 + (g2^11*t^4.348)/g1 + g1*g2^5*t^4.428 + (g2^4*t^4.452)/g1^4 + t^4.532/(g1^2*g2^2) + (2*t^4.612)/g2^8 + (g1^2*t^4.692)/g2^14 + (g2^8*t^4.767)/g1^2 + (g1^4*t^4.772)/g2^20 + 2*g2^2*t^4.847 + (g1^2*t^4.927)/g2^4 + g2^12*t^5.082 + (2*g2^5*t^5.186)/g1^3 + t^5.266/(g1*g2) + (g1*t^5.346)/g2^7 + (2*g2^9*t^5.501)/g1 + (3*g2^6*t^5.92)/g1^2 - 2*t^6. + g2^10*t^6.235 - t^6.419/(g1*g2^3) - (g1*t^6.499)/g2^9 + (g2^13*t^6.574)/g1^3 + (2*g2^7*t^6.654)/g1 + (g2^6*t^6.678)/g1^6 + t^6.758/g1^4 + (g1^3*t^6.814)/g2^5 + (2*t^6.838)/(g1^2*g2^6) + (g2^17*t^6.889)/g1 + (2*t^6.918)/g2^12 + g1*g2^11*t^6.969 + (g2^10*t^6.993)/g1^4 + (2*g1^2*t^6.998)/g2^18 + (g2^4*t^7.073)/g1^2 + (g1^4*t^7.078)/g2^24 + t^7.153/g2^2 + (g1^6*t^7.159)/g2^30 + (g1^2*t^7.233)/g2^8 + (2*g2^14*t^7.308)/g1^2 + (g1^4*t^7.313)/g2^14 + 2*g2^8*t^7.388 + (2*g2^7*t^7.412)/g1^5 + (g2*t^7.492)/g1^3 + (2*t^7.572)/(g1*g2^5) + g2^18*t^7.623 + (2*g2^11*t^7.727)/g1^3 + (g1^3*t^7.732)/g2^17 + (g2^5*t^7.807)/g1 - (g1*t^7.887)/g2 + (2*g2^15*t^8.042)/g1 + (3*g2^8*t^8.146)/g1^4 - (2*g2^2*t^8.226)/g1^2 - t^8.306/g2^4 - (3*g1^2*t^8.386)/g2^10 + (2*g2^12*t^8.461)/g1^2 - 3*g2^6*t^8.541 - g1^2*t^8.621 - t^8.645/(g1^3*g2) + (g2^22*t^8.696)/g1^2 - t^8.725/(g1*g2^7) + 2*g2^16*t^8.776 + (g2^15*t^8.8)/g1^5 - (g1*t^8.805)/g2^13 + g1^2*g2^10*t^8.856 + (4*g2^9*t^8.88)/g1^3 - (g1^3*t^8.885)/g2^19 + (g2^8*t^8.904)/g1^8 - (5*g2^3*t^8.96)/g1 + (g2^2*t^8.984)/g1^6 - t^4.153/(g2^2*y) - t^6.379/(g1^2*y) - t^6.459/(g2^6*y) - (g1^2*t^6.539)/(g2^12*y) - (g2*t^7.113)/(g1*y) + (g1*t^7.193)/(g2^5*y) + t^7.532/(g1^2*g2^2*y) + t^7.612/(g2^8*y) + (g1^2*t^7.692)/(g2^14*y) + (2*g2^8*t^7.767)/(g1^2*y) + (2*g2^2*t^7.847)/y + (2*g1^2*t^7.927)/(g2^4*y) + (2*g2^5*t^8.186)/(g1^3*y) + (2*t^8.266)/(g1*g2*y) + (2*g1*t^8.346)/(g2^7*y) + (2*g2^9*t^8.501)/(g1*y) - (g2^2*t^8.605)/(g1^4*y) - t^8.685/(g1^2*g2^4*y) - (2*t^8.765)/(g2^10*y) - (g1^2*t^8.845)/(g2^16*y) + (2*g2^6*t^8.92)/(g1^2*y) - (g1^4*t^8.925)/(g2^22*y) - (t^4.153*y)/g2^2 - (t^6.379*y)/g1^2 - (t^6.459*y)/g2^6 - (g1^2*t^6.539*y)/g2^12 - (g2*t^7.113*y)/g1 + (g1*t^7.193*y)/g2^5 + (t^7.532*y)/(g1^2*g2^2) + (t^7.612*y)/g2^8 + (g1^2*t^7.692*y)/g2^14 + (2*g2^8*t^7.767*y)/g1^2 + 2*g2^2*t^7.847*y + (2*g1^2*t^7.927*y)/g2^4 + (2*g2^5*t^8.186*y)/g1^3 + (2*t^8.266*y)/(g1*g2) + (2*g1*t^8.346*y)/g2^7 + (2*g2^9*t^8.501*y)/g1 - (g2^2*t^8.605*y)/g1^4 - (t^8.685*y)/(g1^2*g2^4) - (2*t^8.765*y)/g2^10 - (g1^2*t^8.845*y)/g2^16 + (2*g2^6*t^8.92*y)/g1^2 - (g1^4*t^8.925*y)/g2^22


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
48156 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{3}^{2}$ 0.566 0.7123 0.7946 [M:[0.9205, 1.0795, 1.0, 0.682, 1.0795], q:[0.6307, 0.4488], qb:[0.2898, 0.9488], phi:[0.4205]] t^2.046 + t^2.216 + t^2.523 + t^3. + 2*t^3.239 + t^3.477 + t^3.716 + t^4.092 + t^4.193 + t^4.261 + t^4.431 + t^4.569 + 2*t^4.739 + 2*t^5.046 + t^5.216 + t^5.284 + 2*t^5.454 + t^5.523 + t^5.693 + 2*t^5.761 + t^5.931 - t^6. - t^4.261/y - t^4.261*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
46335 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ 0.6052 0.7542 0.8024 [M:[1.0, 1.0, 0.7685, 0.7685], q:[0.5764, 0.4236], qb:[0.4236, 1.0393], phi:[0.3843]] 3*t^2.306 + t^2.542 + 2*t^3. + t^3.694 + 2*t^4.389 + 6*t^4.611 + 4*t^4.847 + t^5.083 + 4*t^5.306 + 2*t^5.542 + t^6. - t^4.153/y - t^4.153*y detail