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
2985 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ 0.576 0.7183 0.8019 [X:[1.5743], M:[0.4257, 1.2772, 0.7228, 0.9801, 1.0199, 0.8515], q:[0.9357, 0.6386], qb:[0.3415, 0.3813], phi:[0.4257]] [X:[[2]], M:[[-2], [-6], [6], [-14], [14], [-4]], q:[[5], [-3]], qb:[[-11], [17]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{3}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$ ${}$ -1 t^2.168 + 2*t^2.554 + t^2.94 + t^3.06 + t^3.326 + t^3.565 + t^3.832 + t^3.951 + t^4.337 + 3*t^4.723 + 4*t^5.109 + t^5.228 + 2*t^5.495 + t^5.614 + t^5.733 + 2*t^5.881 - t^6. + 3*t^6.119 + t^6.267 + t^6.386 + 2*t^6.505 + t^6.625 + t^6.653 - t^6.772 + 2*t^6.891 + t^7.13 + 4*t^7.277 + t^7.516 + 6*t^7.663 + t^7.782 + 2*t^7.902 + 3*t^8.049 - 2*t^8.168 + 3*t^8.288 + 3*t^8.435 - 4*t^8.554 + 4*t^8.674 + t^8.793 + 2*t^8.821 - 2*t^8.94 - t^4.277/y - (2*t^6.832)/y + (4*t^7.723)/y + (2*t^8.109)/y + t^8.228/y + (3*t^8.495)/y + (2*t^8.614)/y + t^8.733/y + (2*t^8.881)/y - t^4.277*y - 2*t^6.832*y + 4*t^7.723*y + 2*t^8.109*y + t^8.228*y + 3*t^8.495*y + 2*t^8.614*y + t^8.733*y + 2*t^8.881*y g1^6*t^2.168 + (2*t^2.554)/g1^4 + t^2.94/g1^14 + g1^14*t^3.06 + t^3.326/g1^24 + g1^32*t^3.565 + t^3.832/g1^6 + g1^22*t^3.951 + g1^12*t^4.337 + 3*g1^2*t^4.723 + (4*t^5.109)/g1^8 + g1^20*t^5.228 + (2*t^5.495)/g1^18 + g1^10*t^5.614 + g1^38*t^5.733 + (2*t^5.881)/g1^28 - t^6. + 3*g1^28*t^6.119 + t^6.267/g1^38 + t^6.386/g1^10 + 2*g1^18*t^6.505 + g1^46*t^6.625 + t^6.653/g1^48 - t^6.772/g1^20 + 2*g1^8*t^6.891 + g1^64*t^7.13 + (4*t^7.277)/g1^2 + g1^54*t^7.516 + (6*t^7.663)/g1^12 + g1^16*t^7.782 + 2*g1^44*t^7.902 + (3*t^8.049)/g1^22 - 2*g1^6*t^8.168 + 3*g1^34*t^8.288 + (3*t^8.435)/g1^32 - (4*t^8.554)/g1^4 + 4*g1^24*t^8.674 + g1^52*t^8.793 + (2*t^8.821)/g1^42 - (2*t^8.94)/g1^14 - t^4.277/(g1^2*y) - (2*t^6.832)/(g1^6*y) + (4*g1^2*t^7.723)/y + (2*t^8.109)/(g1^8*y) + (g1^20*t^8.228)/y + (3*t^8.495)/(g1^18*y) + (2*g1^10*t^8.614)/y + (g1^38*t^8.733)/y + (2*t^8.881)/(g1^28*y) - (t^4.277*y)/g1^2 - (2*t^6.832*y)/g1^6 + 4*g1^2*t^7.723*y + (2*t^8.109*y)/g1^8 + g1^20*t^8.228*y + (3*t^8.495*y)/g1^18 + 2*g1^10*t^8.614*y + g1^38*t^8.733*y + (2*t^8.881*y)/g1^28


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
3594 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ 0.5735 0.715 0.8022 [X:[1.5789], M:[0.4211, 1.2632, 0.7368, 0.9474, 1.0526, 0.8421], q:[0.9474, 0.6316], qb:[0.3158, 0.4211], phi:[0.4211]] t^2.211 + 2*t^2.526 + t^2.842 + 2*t^3.158 + 2*t^3.789 + t^4.105 + t^4.421 + 3*t^4.737 + 4*t^5.053 + 3*t^5.368 + 3*t^5.684 + t^6. - t^4.263/y - t^4.263*y detail {a: 62943/109744, c: 39233/54872, X1: 30/19, M1: 8/19, M2: 24/19, M3: 14/19, M4: 18/19, M5: 20/19, M6: 16/19, q1: 18/19, q2: 12/19, qb1: 6/19, qb2: 8/19, phi1: 8/19}


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
1945 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ 0.563 0.6963 0.8086 [X:[1.5736], M:[0.4264, 1.2792, 0.7208, 0.9848, 1.0152], q:[0.934, 0.6396], qb:[0.3452, 0.3756], phi:[0.4264]] t^2.162 + t^2.558 + t^2.954 + t^3.046 + t^3.35 + t^3.442 + t^3.533 + t^3.838 + t^3.929 + t^4.325 + 2*t^4.721 + 2*t^5.117 + t^5.208 + t^5.513 + t^5.604 + t^5.695 + t^5.909 - t^4.279/y - t^4.279*y detail