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
8733 Sp2adj1nf1 $\phi_1^2X_1$ + $ \phi_1q_1^2q_2^2$ + $ M_1\phi_1q_1q_2$ + $ M_2\phi_1q_1^2$ + $ M_2\phi_1^4$ + $ M_3\phi_1^3q_1^2$ 1.0334 1.1471 0.9009 [X:[1.6364], M:[0.9091, 1.2727, 0.9091], q:[0.2727, 0.6364], qb:[], phi:[0.1818]] [X:[[0]], M:[[0], [0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 2751/2662, c: 6107/5324, X1: 18/11, M1: 10/11, M2: 14/11, M3: 10/11, q1: 3/11, q2: 7/11, phi1: 2/11}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1^4$, $ M_1$, $ M_3$, $ q_1q_2$, $ M_2$, $ \phi_1^2q_1q_2$, $ \phi_1^8$, $ \phi_1^3q_1q_2$, $ \phi_1q_2^2$, $ M_1\phi_1^4$, $ M_3\phi_1^4$, $ \phi_1^4q_1q_2$, $ X_1$, $ M_1^2$, $ M_1M_3$, $ M_3^2$, $ M_1q_1q_2$, $ M_3q_1q_2$, $ \phi_1^3q_2^2$, $ q_1^2q_2^2$ $\phi_1^6q_1q_2$ -1 t^2.18 + 3*t^2.73 + 2*t^3.82 + 3*t^4.36 + 3*t^4.91 + 6*t^5.45 - t^6. + 7*t^6.55 + 6*t^7.09 + 6*t^7.64 + 12*t^8.18 - 3*t^8.73 + t^8.18/y^2 - t^8.73/y^2 - t^3.55/y - t^4.64/y - t^5.73/y - (3*t^6.27)/y - (4*t^7.36)/y + (2*t^7.91)/y - t^3.55*y - t^4.64*y - t^5.73*y - 3*t^6.27*y - 4*t^7.36*y + 2*t^7.91*y + t^8.18*y^2 - t^8.73*y^2 t^2.18 + 3*t^2.73 + 2*t^3.82 + 3*t^4.36 + 3*t^4.91 + 6*t^5.45 - t^6. + 7*t^6.55 + 6*t^7.09 + 6*t^7.64 + 12*t^8.18 - 3*t^8.73 + t^8.18/y^2 - t^8.73/y^2 - t^3.55/y - t^4.64/y - t^5.73/y - (3*t^6.27)/y - (4*t^7.36)/y + (2*t^7.91)/y - t^3.55*y - t^4.64*y - t^5.73*y - 3*t^6.27*y - 4*t^7.36*y + 2*t^7.91*y + t^8.18*y^2 - t^8.73*y^2


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
8864 $\phi_1^2X_1$ + $ \phi_1q_1^2q_2^2$ + $ M_1\phi_1q_1q_2$ + $ M_2\phi_1q_1^2$ + $ M_2\phi_1^4$ + $ M_3\phi_1^3q_1^2$ + $ M_2M_4$ 1.0533 1.184 0.8896 [X:[1.6364], M:[0.9091, 1.2727, 0.9091, 0.7273], q:[0.2727, 0.6364], qb:[], phi:[0.1818]] 2*t^2.18 + 3*t^2.73 + t^3.82 + 5*t^4.36 + 6*t^4.91 + 6*t^5.45 - t^6. - t^3.55/y - t^4.64/y - (2*t^5.73)/y - t^3.55*y - t^4.64*y - 2*t^5.73*y detail {a: 22431/21296, c: 12607/10648, X1: 18/11, M1: 10/11, M2: 14/11, M3: 10/11, M4: 8/11, q1: 3/11, q2: 7/11, phi1: 2/11}


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
8552 Sp2adj1nf1 $\phi_1^2X_1$ + $ \phi_1q_1^2q_2^2$ + $ M_1\phi_1q_1q_2$ + $ M_2\phi_1q_1^2$ + $ M_2\phi_1^4$ 1.0251 1.1331 0.9047 [X:[1.6364], M:[0.9091, 1.2727], q:[0.2727, 0.6364], qb:[], phi:[0.1818]] t^2.18 + 2*t^2.73 + t^3.27 + 2*t^3.82 + 3*t^4.36 + 2*t^4.91 + 4*t^5.45 + t^6. - t^3.55/y - t^4.64/y - t^5.73/y - t^3.55*y - t^4.64*y - t^5.73*y detail {a: 21831/21296, c: 12065/10648, X1: 18/11, M1: 10/11, M2: 14/11, q1: 3/11, q2: 7/11, phi1: 2/11}