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
50996 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{4}M_{6}$ 0.7012 0.8624 0.8131 [M:[1.0226, 0.8868, 0.9321, 1.0679, 1.0226, 0.9321], q:[0.534, 0.4434], qb:[0.5793, 0.4887], phi:[0.4887]] [M:[[-2], [10], [6], [-6], [-2], [6]], q:[[-3], [5]], qb:[[-7], [1]], phi:[[1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{6}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$ ${}$ -4 t^2.66 + 2*t^2.796 + 4*t^3.068 + t^4.126 + t^4.262 + 2*t^4.398 + 2*t^4.534 + 2*t^4.67 + t^4.806 + t^4.942 + t^5.321 + 2*t^5.457 + 2*t^5.592 + 2*t^5.728 + 5*t^5.864 - 4*t^6. + 6*t^6.136 - 2*t^6.272 - t^6.408 + t^6.787 + 3*t^6.923 + 3*t^7.058 + 6*t^7.194 + 4*t^7.33 + 5*t^7.466 + 3*t^7.602 + 3*t^7.738 + t^7.981 + 2*t^8.01 + 2*t^8.117 + 3*t^8.253 + 5*t^8.389 + 4*t^8.524 + 3*t^8.66 - 3*t^8.796 + 6*t^8.932 - t^4.466/y - t^7.126/y - t^7.262/y + t^7.398/y - t^7.534/y + t^7.67/y + t^7.806/y + (2*t^8.457)/y + t^8.592/y + (4*t^8.728)/y + (8*t^8.864)/y - t^4.466*y - t^7.126*y - t^7.262*y + t^7.398*y - t^7.534*y + t^7.67*y + t^7.806*y + 2*t^8.457*y + t^8.592*y + 4*t^8.728*y + 8*t^8.864*y g1^10*t^2.66 + 2*g1^6*t^2.796 + (4*t^3.068)/g1^2 + g1^11*t^4.126 + g1^7*t^4.262 + 2*g1^3*t^4.398 + (2*t^4.534)/g1 + (2*t^4.67)/g1^5 + t^4.806/g1^9 + t^4.942/g1^13 + g1^20*t^5.321 + 2*g1^16*t^5.457 + 2*g1^12*t^5.592 + 2*g1^8*t^5.728 + 5*g1^4*t^5.864 - 4*t^6. + (6*t^6.136)/g1^4 - (2*t^6.272)/g1^8 - t^6.408/g1^12 + g1^21*t^6.787 + 3*g1^17*t^6.923 + 3*g1^13*t^7.058 + 6*g1^9*t^7.194 + 4*g1^5*t^7.33 + 5*g1*t^7.466 + (3*t^7.602)/g1^3 + (3*t^7.738)/g1^7 + g1^30*t^7.981 + (2*t^8.01)/g1^15 + 2*g1^26*t^8.117 + 3*g1^22*t^8.253 + 5*g1^18*t^8.389 + 4*g1^14*t^8.524 + 3*g1^10*t^8.66 - 3*g1^6*t^8.796 + 6*g1^2*t^8.932 - (g1*t^4.466)/y - (g1^11*t^7.126)/y - (g1^7*t^7.262)/y + (g1^3*t^7.398)/y - t^7.534/(g1*y) + t^7.67/(g1^5*y) + t^7.806/(g1^9*y) + (2*g1^16*t^8.457)/y + (g1^12*t^8.592)/y + (4*g1^8*t^8.728)/y + (8*g1^4*t^8.864)/y - g1*t^4.466*y - g1^11*t^7.126*y - g1^7*t^7.262*y + g1^3*t^7.398*y - (t^7.534*y)/g1 + (t^7.67*y)/g1^5 + (t^7.806*y)/g1^9 + 2*g1^16*t^8.457*y + g1^12*t^8.592*y + 4*g1^8*t^8.728*y + 8*g1^4*t^8.864*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
56225 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{4}M_{6}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}X_{1}$ 0.619 0.768 0.8059 [X:[1.3846], M:[1.0769, 0.6154, 0.7692, 1.2308, 1.0769, 0.7692], q:[0.6154, 0.3077], qb:[0.7692, 0.4615], phi:[0.4615]] 2*t^2.308 + 5*t^3.231 + t^3.692 + 3*t^4.154 + 4*t^4.615 + 8*t^5.538 - 2*t^6. - t^4.385/y - t^4.385*y detail {a: 21759/35152, c: 13499/17576, X1: 18/13, M1: 14/13, M2: 8/13, M3: 10/13, M4: 16/13, M5: 14/13, M6: 10/13, q1: 8/13, q2: 4/13, qb1: 10/13, qb2: 6/13, phi1: 6/13}


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
47250 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ 0.6959 0.8526 0.8162 [M:[1.0156, 0.9222, 0.9533, 1.0467, 1.0156], q:[0.5233, 0.4611], qb:[0.5545, 0.4922], phi:[0.4922]] t^2.767 + t^2.86 + 4*t^3.047 + t^3.14 + t^4.243 + t^4.337 + 2*t^4.43 + 2*t^4.523 + 2*t^4.617 + t^4.71 + t^4.804 + t^5.533 + t^5.626 + 2*t^5.813 + 2*t^5.907 - 3*t^6. - t^4.477/y - t^4.477*y detail