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
56546 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}M_{6}$ + ${ }M_{2}M_{7}$ 0.6679 0.8314 0.8034 [M:[1.154, 1.0768, 0.846, 0.7695, 0.6924, 1.2305, 0.9232], q:[0.3848, 0.4613], qb:[0.5384, 0.7692], phi:[0.4616]] [M:[[-5], [4], [5], [-12], [-3], [12], [-4]], q:[[-6], [11]], qb:[[2], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }M_{3}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}M_{6}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ ${}M_{5}\tilde{q}_{1}\tilde{q}_{2}$ -1 t^2.077 + t^2.538 + 2*t^2.77 + t^2.999 + t^3.462 + t^3.691 + t^3.693 + t^3.923 + t^4.152 + 2*t^4.154 + t^4.384 + 2*t^4.615 + 2*t^4.847 + 2*t^5.076 + 2*t^5.308 + t^5.537 + 3*t^5.539 + 2*t^5.769 + t^5.998 - t^6. + t^6.23 + 3*t^6.231 + 2*t^6.461 + 2*t^6.463 + 2*t^6.691 + 3*t^6.692 + 3*t^6.922 + 2*t^6.924 + t^7.152 + 3*t^7.153 + t^7.383 + 2*t^7.385 + t^7.387 + 2*t^7.614 + 3*t^7.616 + t^7.844 + 3*t^7.846 + t^7.848 + 3*t^8.075 + t^8.077 + t^8.305 + 2*t^8.307 + 5*t^8.309 + 2*t^8.536 + 4*t^8.768 - t^8.77 + t^8.997 - t^4.385/y - t^6.462/y - t^7.154/y + (2*t^7.615)/y + (2*t^7.847)/y + t^8.076/y + (3*t^8.308)/y + t^8.537/y + t^8.539/y + (3*t^8.769)/y + t^8.77/y - t^4.385*y - t^6.462*y - t^7.154*y + 2*t^7.615*y + 2*t^7.847*y + t^8.076*y + 3*t^8.308*y + t^8.537*y + t^8.539*y + 3*t^8.769*y + t^8.77*y t^2.077/g1^3 + g1^5*t^2.538 + (2*t^2.77)/g1^4 + g1^13*t^2.999 + t^3.462/g1^5 + g1^12*t^3.691 + t^3.693/g1^14 + g1^3*t^3.923 + g1^20*t^4.152 + (2*t^4.154)/g1^6 + g1^11*t^4.384 + 2*g1^2*t^4.615 + (2*t^4.847)/g1^7 + 2*g1^10*t^5.076 + 2*g1*t^5.308 + g1^18*t^5.537 + (3*t^5.539)/g1^8 + 2*g1^9*t^5.769 + g1^26*t^5.998 - t^6. + g1^17*t^6.23 + (3*t^6.231)/g1^9 + 2*g1^8*t^6.461 + (2*t^6.463)/g1^18 + 2*g1^25*t^6.691 + (3*t^6.692)/g1 + 3*g1^16*t^6.922 + (2*t^6.924)/g1^10 + g1^33*t^7.152 + 3*g1^7*t^7.153 + g1^24*t^7.383 + (2*t^7.385)/g1^2 + t^7.387/g1^28 + 2*g1^15*t^7.614 + (3*t^7.616)/g1^11 + g1^32*t^7.844 + 3*g1^6*t^7.846 + t^7.848/g1^20 + 3*g1^23*t^8.075 + t^8.077/g1^3 + g1^40*t^8.305 + 2*g1^14*t^8.307 + (5*t^8.309)/g1^12 + 2*g1^31*t^8.536 + 4*g1^22*t^8.768 - t^8.77/g1^4 + g1^39*t^8.997 - t^4.385/(g1^2*y) - t^6.462/(g1^5*y) - t^7.154/(g1^6*y) + (2*g1^2*t^7.615)/y + (2*t^7.847)/(g1^7*y) + (g1^10*t^8.076)/y + (3*g1*t^8.308)/y + (g1^18*t^8.537)/y + t^8.539/(g1^8*y) + (3*g1^9*t^8.769)/y + t^8.77/(g1^17*y) - (t^4.385*y)/g1^2 - (t^6.462*y)/g1^5 - (t^7.154*y)/g1^6 + 2*g1^2*t^7.615*y + (2*t^7.847*y)/g1^7 + g1^10*t^8.076*y + 3*g1*t^8.308*y + g1^18*t^8.537*y + (t^8.539*y)/g1^8 + 3*g1^9*t^8.769*y + (t^8.77*y)/g1^17


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
53796 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}M_{6}$ 0.661 0.8205 0.8057 [M:[1.1596, 1.0724, 0.8404, 0.7829, 0.6957, 1.2171], q:[0.3915, 0.449], qb:[0.5362, 0.7681], phi:[0.4638]] t^2.087 + t^2.521 + t^2.783 + t^2.955 + t^3.217 + t^3.479 + t^3.651 + t^3.74 + t^3.913 + t^4.085 + 2*t^4.174 + t^4.347 + 2*t^4.609 + t^4.87 + 2*t^5.043 + 2*t^5.304 + t^5.477 + t^5.566 + 2*t^5.738 + t^5.911 - t^4.391/y - t^4.391*y detail