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
50948 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ 0.6644 0.8389 0.792 [M:[1.1879, 0.8121, 0.8121, 0.7717, 0.7717, 0.8324], q:[0.3858, 0.4263], qb:[0.802, 0.802], phi:[0.396]] [M:[[-6], [6], [6], [-14], [-14], [16]], q:[[-7], [13]], qb:[[1], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}q_{1}q_{2}$, ${ }M_{5}\phi_{1}q_{1}q_{2}$ ${}M_{1}M_{2}$, ${ }\phi_{1}^{3}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$ 0 2*t^2.315 + t^2.376 + 2*t^2.436 + t^2.497 + t^3.564 + t^3.624 + t^3.746 + 3*t^4.63 + 2*t^4.691 + 5*t^4.751 + 5*t^4.812 + 4*t^4.873 + 2*t^4.934 + t^4.994 + t^5.879 + t^5.939 + 3*t^6.061 + t^6.121 + 2*t^6.182 + t^6.243 + 4*t^6.945 + 3*t^7.006 + 7*t^7.066 + 8*t^7.127 + 8*t^7.188 + 6*t^7.249 + 7*t^7.309 + 4*t^7.37 + 2*t^7.431 + 2*t^7.492 + t^8.193 - 4*t^8.315 - 3*t^8.436 + t^8.497 + 3*t^8.558 + 4*t^8.619 + 2*t^8.679 + t^8.74 - t^4.188/y - (2*t^6.503)/y - t^6.564/y - t^6.624/y - t^6.685/y + t^7.63/y + (3*t^7.691)/y + (5*t^7.751)/y + (5*t^7.812)/y + (4*t^7.873)/y + (2*t^7.934)/y - (3*t^8.818)/y - t^4.188*y - 2*t^6.503*y - t^6.564*y - t^6.624*y - t^6.685*y + t^7.63*y + 3*t^7.691*y + 5*t^7.751*y + 5*t^7.812*y + 4*t^7.873*y + 2*t^7.934*y - 3*t^8.818*y (2*t^2.315)/g1^14 + t^2.376/g1^4 + 2*g1^6*t^2.436 + g1^16*t^2.497 + t^3.564/g1^6 + g1^4*t^3.624 + g1^24*t^3.746 + (3*t^4.63)/g1^28 + (2*t^4.691)/g1^18 + (5*t^4.751)/g1^8 + 5*g1^2*t^4.812 + 4*g1^12*t^4.873 + 2*g1^22*t^4.934 + g1^32*t^4.994 + t^5.879/g1^20 + t^5.939/g1^10 + 3*g1^10*t^6.061 + g1^20*t^6.121 + 2*g1^30*t^6.182 + g1^40*t^6.243 + (4*t^6.945)/g1^42 + (3*t^7.006)/g1^32 + (7*t^7.066)/g1^22 + (8*t^7.127)/g1^12 + (8*t^7.188)/g1^2 + 6*g1^8*t^7.249 + 7*g1^18*t^7.309 + 4*g1^28*t^7.37 + 2*g1^38*t^7.431 + 2*g1^48*t^7.492 + t^8.193/g1^34 - (4*t^8.315)/g1^14 - 3*g1^6*t^8.436 + g1^16*t^8.497 + 3*g1^26*t^8.558 + 4*g1^36*t^8.619 + 2*g1^46*t^8.679 + g1^56*t^8.74 - t^4.188/(g1^2*y) - (2*t^6.503)/(g1^16*y) - t^6.564/(g1^6*y) - (g1^4*t^6.624)/y - (g1^14*t^6.685)/y + t^7.63/(g1^28*y) + (3*t^7.691)/(g1^18*y) + (5*t^7.751)/(g1^8*y) + (5*g1^2*t^7.812)/y + (4*g1^12*t^7.873)/y + (2*g1^22*t^7.934)/y - (3*t^8.818)/(g1^30*y) - (t^4.188*y)/g1^2 - (2*t^6.503*y)/g1^16 - (t^6.564*y)/g1^6 - g1^4*t^6.624*y - g1^14*t^6.685*y + (t^7.63*y)/g1^28 + (3*t^7.691*y)/g1^18 + (5*t^7.751*y)/g1^8 + 5*g1^2*t^7.812*y + 4*g1^12*t^7.873*y + 2*g1^22*t^7.934*y - (3*t^8.818*y)/g1^30


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
56087 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{7}\phi_{1}q_{1}q_{2}$ 0.6814 0.8689 0.7842 [M:[1.1858, 0.8142, 0.8142, 0.767, 0.767, 0.8378, 0.7906], q:[0.3835, 0.4307], qb:[0.8024, 0.8024], phi:[0.3953]] 2*t^2.301 + 2*t^2.372 + 2*t^2.442 + t^2.513 + t^3.558 + t^3.77 + 3*t^4.602 + 4*t^4.673 + 7*t^4.743 + 7*t^4.814 + 5*t^4.885 + 2*t^4.956 + t^5.027 + t^5.858 - t^6. - t^4.186/y - t^4.186*y detail
56086 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{7}\phi_{1}^{2}$ 0.6475 0.8091 0.8002 [M:[1.1899, 0.8101, 0.8101, 0.7764, 0.7764, 0.827, 1.2067], q:[0.3882, 0.4219], qb:[0.8017, 0.8017], phi:[0.3966]] 2*t^2.329 + 2*t^2.43 + t^2.481 + t^3.57 + 2*t^3.62 + t^3.721 + 3*t^4.658 + 4*t^4.76 + 3*t^4.81 + 3*t^4.861 + 2*t^4.911 + t^4.962 + t^5.899 + 2*t^5.949 - t^6. - t^4.19/y - t^4.19*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
48168 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ 0.6733 0.8548 0.7876 [M:[1.1492, 0.7116, 0.8508, 0.8206, 0.6814, 0.7963], q:[0.4103, 0.4405], qb:[0.8781, 0.7389], phi:[0.3831]] t^2.044 + t^2.135 + t^2.298 + t^2.389 + t^2.462 + t^2.552 + t^3.448 + t^3.702 + t^3.792 + t^4.088 + t^4.179 + t^4.27 + t^4.343 + 2*t^4.433 + t^4.506 + t^4.524 + 3*t^4.597 + 2*t^4.687 + t^4.76 + t^4.778 + 3*t^4.851 + t^4.924 + t^4.941 + t^5.014 + t^5.105 + t^5.492 + t^5.582 + t^5.746 + 2*t^5.836 + t^5.927 - t^6. - t^4.149/y - t^4.149*y detail