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
46393 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ 0.6384 0.7923 0.8057 [M:[0.7685, 1.1527, 0.8473, 0.6897], q:[0.8473, 0.3842], qb:[0.463, 0.7685], phi:[0.3842]] [M:[[2], [3], [-3], [7]], q:[[-3], [1]], qb:[[-4], [2]], phi:[[1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{4}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ ${}M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ 2 t^2.069 + 2*t^2.305 + t^2.542 + 2*t^3.458 + 2*t^3.695 + t^3.931 + t^4.138 + 2*t^4.375 + 4*t^4.611 + 3*t^4.847 + t^5.084 + 2*t^5.527 + 4*t^5.764 + 2*t^6. + t^6.208 + 2*t^6.236 + 2*t^6.444 + t^6.473 + 4*t^6.68 + 8*t^6.916 + 4*t^7.153 + t^7.389 + 2*t^7.597 + t^7.625 + 4*t^7.833 + t^7.862 + 4*t^8.069 + t^8.277 + t^8.305 + 2*t^8.513 - t^8.542 + 4*t^8.749 + t^8.778 + 8*t^8.986 - t^4.153/y - t^6.222/y - (2*t^6.458)/y + (2*t^7.375)/y + (2*t^7.611)/y + (4*t^7.847)/y + t^8.084/y - t^8.291/y + (3*t^8.764)/y - t^4.153*y - t^6.222*y - 2*t^6.458*y + 2*t^7.375*y + 2*t^7.611*y + 4*t^7.847*y + t^8.084*y - t^8.291*y + 3*t^8.764*y g1^7*t^2.069 + 2*g1^2*t^2.305 + t^2.542/g1^3 + 2*g1^3*t^3.458 + (2*t^3.695)/g1^2 + t^3.931/g1^7 + g1^14*t^4.138 + 2*g1^9*t^4.375 + 4*g1^4*t^4.611 + (3*t^4.847)/g1 + t^5.084/g1^6 + 2*g1^10*t^5.527 + 4*g1^5*t^5.764 + 2*t^6. + g1^21*t^6.208 + (2*t^6.236)/g1^5 + 2*g1^16*t^6.444 + t^6.473/g1^10 + 4*g1^11*t^6.68 + 8*g1^6*t^6.916 + 4*g1*t^7.153 + t^7.389/g1^4 + 2*g1^17*t^7.597 + t^7.625/g1^9 + 4*g1^12*t^7.833 + t^7.862/g1^14 + 4*g1^7*t^8.069 + g1^28*t^8.277 + g1^2*t^8.305 + 2*g1^23*t^8.513 - t^8.542/g1^3 + 4*g1^18*t^8.749 + t^8.778/g1^8 + 8*g1^13*t^8.986 - (g1*t^4.153)/y - (g1^8*t^6.222)/y - (2*g1^3*t^6.458)/y + (2*g1^9*t^7.375)/y + (2*g1^4*t^7.611)/y + (4*t^7.847)/(g1*y) + t^8.084/(g1^6*y) - (g1^15*t^8.291)/y + (3*g1^5*t^8.764)/y - g1*t^4.153*y - g1^8*t^6.222*y - 2*g1^3*t^6.458*y + 2*g1^9*t^7.375*y + 2*g1^4*t^7.611*y + (4*t^7.847*y)/g1 + (t^8.084*y)/g1^6 - g1^15*t^8.291*y + 3*g1^5*t^8.764*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
46889 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}^{2}$ 0.5751 0.7179 0.801 [M:[0.8571, 1.2857, 0.7143, 1.0], q:[0.7143, 0.4286], qb:[0.2857, 0.8571], phi:[0.4286]] t^2.143 + 2*t^2.571 + 2*t^3. + 2*t^3.429 + 2*t^3.857 + t^4.286 + 3*t^4.714 + 5*t^5.143 + 4*t^5.571 + 4*t^6. - t^4.286/y - t^4.286*y detail {a: 789/1372, c: 985/1372, M1: 6/7, M2: 9/7, M3: 5/7, M4: 1, q1: 5/7, q2: 3/7, qb1: 2/7, qb2: 6/7, phi1: 3/7}
48240 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ 0.6591 0.8331 0.7912 [M:[0.7667, 1.15, 0.85, 0.6833, 0.6833], q:[0.85, 0.3833], qb:[0.4667, 0.7667], phi:[0.3833]] 2*t^2.05 + 2*t^2.3 + t^2.55 + 2*t^3.45 + 2*t^3.7 + 3*t^4.1 + 4*t^4.35 + 5*t^4.6 + 3*t^4.85 + t^5.1 + 4*t^5.5 + 6*t^5.75 + t^6. - t^4.15/y - t^4.15*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
46307 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ 0.6178 0.7527 0.8207 [M:[0.7725, 1.1587, 0.8413], q:[0.8413, 0.3862], qb:[0.455, 0.7725], phi:[0.3862]] 2*t^2.317 + t^2.524 + 2*t^3.476 + 2*t^3.683 + 2*t^3.889 + 3*t^4.635 + 3*t^4.841 + t^5.048 + 2*t^5.794 + t^6. - t^4.159/y - t^4.159*y detail