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
2428 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}q_{1}\tilde{q}_{1}$ 0.6101 0.7833 0.7789 [M:[0.9726, 1.0823, 1.0274, 0.9177, 0.7431, 1.2569, 0.798], q:[0.7431, 0.2843], qb:[0.4589, 0.4589], phi:[0.5137]] [M:[[4], [-12], [-4], [12], [1], [-1], [-7]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{7}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{7}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ ${}M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ 0 2*t^2.229 + t^2.394 + t^2.753 + 2*t^3.082 + t^3.247 + t^3.606 + 2*t^3.771 + 3*t^4.294 + 3*t^4.459 + 2*t^4.623 + t^4.788 + 2*t^4.983 + t^5.147 + 4*t^5.312 + 2*t^5.476 + t^5.506 + t^5.641 + 3*t^5.835 + 3*t^6.165 + 2*t^6.329 + t^6.359 + t^6.494 + 4*t^6.524 + 5*t^6.688 + 4*t^6.853 + 2*t^7.017 + 3*t^7.047 + t^7.182 + t^7.212 + 5*t^7.377 + 5*t^7.541 + 3*t^7.706 + 2*t^7.736 + 2*t^7.87 + 2*t^7.9 + t^8.035 + 5*t^8.065 - 3*t^8.229 + t^8.259 + 2*t^8.394 + 3*t^8.559 + 8*t^8.589 + 2*t^8.723 + t^8.753 + t^8.888 + 5*t^8.918 - t^4.541/y - t^6.935/y + (2*t^7.459)/y + t^7.623/y + (2*t^7.983)/y + (2*t^8.147)/y + (4*t^8.312)/y + (4*t^8.476)/y + t^8.641/y + (4*t^8.835)/y - t^4.541*y - t^6.935*y + 2*t^7.459*y + t^7.623*y + 2*t^7.983*y + 2*t^8.147*y + 4*t^8.312*y + 4*t^8.476*y + t^8.641*y + 4*t^8.835*y 2*g1*t^2.229 + t^2.394/g1^7 + g1^12*t^2.753 + (2*t^3.082)/g1^4 + t^3.247/g1^12 + g1^7*t^3.606 + (2*t^3.771)/g1 + 3*g1^10*t^4.294 + 3*g1^2*t^4.459 + (2*t^4.623)/g1^6 + t^4.788/g1^14 + 2*g1^13*t^4.983 + g1^5*t^5.147 + (4*t^5.312)/g1^3 + (2*t^5.476)/g1^11 + g1^24*t^5.506 + t^5.641/g1^19 + 3*g1^8*t^5.835 + (3*t^6.165)/g1^8 + (2*t^6.329)/g1^16 + g1^19*t^6.359 + t^6.494/g1^24 + 4*g1^11*t^6.524 + 5*g1^3*t^6.688 + (4*t^6.853)/g1^5 + (2*t^7.017)/g1^13 + 3*g1^22*t^7.047 + t^7.182/g1^21 + g1^14*t^7.212 + 5*g1^6*t^7.377 + (5*t^7.541)/g1^2 + (3*t^7.706)/g1^10 + 2*g1^25*t^7.736 + (2*t^7.87)/g1^18 + 2*g1^17*t^7.9 + t^8.035/g1^26 + 5*g1^9*t^8.065 - 3*g1*t^8.229 + g1^36*t^8.259 + (2*t^8.394)/g1^7 + (3*t^8.559)/g1^15 + 8*g1^20*t^8.589 + (2*t^8.723)/g1^23 + g1^12*t^8.753 + t^8.888/g1^31 + 5*g1^4*t^8.918 - t^4.541/(g1^2*y) - t^6.935/(g1^9*y) + (2*g1^2*t^7.459)/y + t^7.623/(g1^6*y) + (2*g1^13*t^7.983)/y + (2*g1^5*t^8.147)/y + (4*t^8.312)/(g1^3*y) + (4*t^8.476)/(g1^11*y) + t^8.641/(g1^19*y) + (4*g1^8*t^8.835)/y - (t^4.541*y)/g1^2 - (t^6.935*y)/g1^9 + 2*g1^2*t^7.459*y + (t^7.623*y)/g1^6 + 2*g1^13*t^7.983*y + 2*g1^5*t^8.147*y + (4*t^8.312*y)/g1^3 + (4*t^8.476*y)/g1^11 + (t^8.641*y)/g1^19 + 4*g1^8*t^8.835*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
4469 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}q_{1}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ 0.6057 0.7801 0.7765 [M:[0.9474, 1.1579, 1.0526, 0.8421, 0.7368, 1.2632, 0.8421], q:[0.7368, 0.3158], qb:[0.4211, 0.4211], phi:[0.5263]] 2*t^2.211 + 2*t^2.526 + 2*t^3.158 + 2*t^3.474 + 2*t^3.789 + 3*t^4.105 + 3*t^4.421 + 4*t^4.737 + 3*t^5.053 + 4*t^5.368 + 5*t^5.684 + 2*t^6. - t^4.579/y - t^4.579*y detail {a: 66477/109744, c: 42805/54872, M1: 18/19, M2: 22/19, M3: 20/19, M4: 16/19, M5: 14/19, M6: 24/19, M7: 16/19, q1: 14/19, q2: 6/19, qb1: 8/19, qb2: 8/19, phi1: 10/19}
4471 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}q_{1}\tilde{q}_{1}$ + ${ }M_{8}\phi_{1}q_{2}^{2}$ 0.62 0.8023 0.7727 [M:[0.9554, 1.1337, 1.0446, 0.8663, 0.7389, 1.2611, 0.828, 0.8663], q:[0.7389, 0.3057], qb:[0.4331, 0.4331], phi:[0.5223]] 2*t^2.217 + t^2.484 + 2*t^2.599 + 2*t^3.134 + t^3.516 + 2*t^3.783 + 3*t^4.166 + 3*t^4.433 + 2*t^4.701 + 4*t^4.815 + t^4.968 + 2*t^5.083 + 3*t^5.198 + 4*t^5.35 + 5*t^5.733 - t^6. - t^4.567/y - t^4.567*y detail
4472 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}q_{1}\tilde{q}_{1}$ + ${ }M_{8}q_{1}\tilde{q}_{2}$ 0.6271 0.8133 0.771 [M:[0.9796, 1.0612, 1.0204, 0.9388, 0.7449, 1.2551, 0.7857, 0.7857], q:[0.7449, 0.2755], qb:[0.4694, 0.4694], phi:[0.5102]] 2*t^2.235 + 2*t^2.357 + t^2.816 + 2*t^3.061 + t^3.184 + 2*t^3.765 + 3*t^4.347 + 3*t^4.469 + 4*t^4.592 + 3*t^4.714 + 2*t^5.051 + 2*t^5.174 + 4*t^5.296 + 4*t^5.418 + 2*t^5.541 + t^5.633 + t^5.878 - t^6. - t^4.531/y - t^4.531*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
1343 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}M_{6}$ 0.5939 0.7557 0.7859 [M:[0.9644, 1.1068, 1.0356, 0.8932, 0.7411, 1.2589], q:[0.7411, 0.2945], qb:[0.4466, 0.4466], phi:[0.5178]] 2*t^2.223 + t^2.68 + 2*t^3.107 + t^3.32 + 2*t^3.563 + 2*t^3.777 + 3*t^4.233 + 3*t^4.447 + 2*t^4.903 + 4*t^5.33 + t^5.359 + 5*t^5.786 - t^6. - t^4.553/y - t^4.553*y detail