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
1881 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ 0.6963 0.8725 0.7981 [M:[0.7273, 1.0909, 0.9091, 0.7273], q:[0.7727, 0.5], qb:[0.5, 0.4091], phi:[0.4545]] [M:[[0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 14829/21296, c: 4645/5324, M1: 8/11, M2: 12/11, M3: 10/11, M4: 8/11, q1: 17/22, q2: 1/2, qb1: 1/2, qb2: 9/22, phi1: 5/11}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ ${}$ -2 2*t^2.182 + 3*t^2.727 + t^3. + t^3.545 + t^3.818 + 2*t^4.091 + 6*t^4.364 + 6*t^4.909 + 2*t^5.182 + 6*t^5.455 + 3*t^5.727 - 2*t^6. + 4*t^6.273 + 11*t^6.545 + 4*t^6.818 + 15*t^7.091 + t^7.364 + 8*t^7.636 + 6*t^7.909 + 5*t^8.182 + 8*t^8.455 + 7*t^8.727 - t^4.364/y - (2*t^6.545)/y - t^7.091/y + t^7.364/y + t^7.636/y + (6*t^7.909)/y + (4*t^8.182)/y + (3*t^8.455)/y + (2*t^8.727)/y - t^4.364*y - 2*t^6.545*y - t^7.091*y + t^7.364*y + t^7.636*y + 6*t^7.909*y + 4*t^8.182*y + 3*t^8.455*y + 2*t^8.727*y 2*t^2.182 + 3*t^2.727 + t^3. + t^3.545 + t^3.818 + 2*t^4.091 + 6*t^4.364 + 6*t^4.909 + 2*t^5.182 + 6*t^5.455 + 3*t^5.727 - 2*t^6. + 4*t^6.273 + 11*t^6.545 + 4*t^6.818 + 15*t^7.091 + t^7.364 + 8*t^7.636 + 6*t^7.909 + 5*t^8.182 + 8*t^8.455 + 7*t^8.727 - t^4.364/y - (2*t^6.545)/y - t^7.091/y + t^7.364/y + t^7.636/y + (6*t^7.909)/y + (4*t^8.182)/y + (3*t^8.455)/y + (2*t^8.727)/y - t^4.364*y - 2*t^6.545*y - t^7.091*y + t^7.364*y + t^7.636*y + 6*t^7.909*y + 4*t^8.182*y + 3*t^8.455*y + 2*t^8.727*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
2896 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ 0.7162 0.9094 0.7876 [M:[0.7273, 1.0909, 0.9091, 0.7273, 0.7273], q:[0.7727, 0.5], qb:[0.5, 0.4091], phi:[0.4545]] 3*t^2.182 + 3*t^2.727 + t^3. + t^3.545 + 2*t^4.091 + 9*t^4.364 + 9*t^4.909 + 3*t^5.182 + 6*t^5.455 + 4*t^5.727 - 4*t^6. - t^4.364/y - t^4.364*y detail {a: 3813/5324, c: 9683/10648, M1: 8/11, M2: 12/11, M3: 10/11, M4: 8/11, M5: 8/11, q1: 17/22, q2: 1/2, qb1: 1/2, qb2: 9/22, phi1: 5/11}
2897 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ 0.7117 0.8992 0.7915 [M:[0.7273, 1.0909, 0.9091, 0.7273, 0.8182], q:[0.7727, 0.5], qb:[0.5, 0.4091], phi:[0.4545]] 2*t^2.182 + t^2.455 + 3*t^2.727 + t^3. + t^3.818 + 2*t^4.091 + 6*t^4.364 + 2*t^4.636 + 7*t^4.909 + 5*t^5.182 + 7*t^5.455 + t^5.727 - 2*t^6. - t^4.364/y - t^4.364*y detail {a: 3789/5324, c: 19149/21296, M1: 8/11, M2: 12/11, M3: 10/11, M4: 8/11, M5: 9/11, q1: 17/22, q2: 1/2, qb1: 1/2, qb2: 9/22, phi1: 5/11}


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
560 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ 0.7011 0.8806 0.7962 [M:[0.6816, 1.1061, 0.8939, 0.6816], q:[0.7765, 0.5419], qb:[0.4581, 0.4358], phi:[0.4469]] 2*t^2.045 + 2*t^2.682 + t^2.933 + t^3. + t^3.637 + t^3.704 + t^4.022 + 4*t^4.089 + t^4.274 + t^4.341 + t^4.592 + 4*t^4.726 + 2*t^4.978 + 2*t^5.045 + 3*t^5.363 + 2*t^5.615 + 3*t^5.682 + t^5.749 + t^5.866 - 2*t^6. - t^4.341/y - t^4.341*y detail