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
8800 Sp2adj1nf1 $\phi_1^2X_1$ + $ M_1q_1q_2$ + $ M_2\phi_1q_1^2$ + $ M_3\phi_1q_1q_2$ + $ M_2M_3$ + $ \phi_1q_2^2$ + $ \phi_1^4X_2$ + $ M_3X_3$ 0.7353 0.7687 0.9566 [X:[1.7333, 1.4667, 1.3333], M:[0.8, 1.3333, 0.6667], q:[0.2667, 0.9333], qb:[], phi:[0.1333]] [X:[[0], [0], [0]], M:[[0], [0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 1103/1500, c: 1153/1500, X1: 26/15, X2: 22/15, X3: 4/3, M1: 4/5, M2: 4/3, M3: 2/3, q1: 4/15, q2: 14/15, phi1: 2/15}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ \phi_1^3q_1^2$, $ M_2$, $ X_3$, $ \phi_1^2q_1q_2$, $ X_2$, $ M_1^2$, $ \phi_1^3q_1q_2$, $ X_1$, $ \phi_1^6q_1^4$ . -1 t^2.4 + t^2.8 + t^4. + t^4.4 + t^4.8 + t^5.2 + t^5.6 - t^6. + t^6.4 + 2*t^6.8 + t^7.2 + 2*t^7.6 + t^8. + t^8.4 - t^8.8 + t^7.6/y^2 - t^8.8/y^2 - t^3.4/y - t^4.2/y - t^5.8/y - t^6.6/y - t^7.4/y - t^8.2/y - t^3.4*y - t^4.2*y - t^5.8*y - t^6.6*y - t^7.4*y - t^8.2*y + t^7.6*y^2 - t^8.8*y^2 t^2.4 + t^2.8 + t^4. + t^4.4 + t^4.8 + t^5.2 + t^5.6 - t^6. + t^6.4 + 2*t^6.8 + t^7.2 + 2*t^7.6 + t^8. + t^8.4 - t^8.8 + t^7.6/y^2 - t^8.8/y^2 - t^3.4/y - t^4.2/y - t^5.8/y - t^6.6/y - t^7.4/y - t^8.2/y - t^3.4*y - t^4.2*y - t^5.8*y - t^6.6*y - t^7.4*y - t^8.2*y + t^7.6*y^2 - t^8.8*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


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
8613 Sp2adj1nf1 $\phi_1^2X_1$ + $ M_1q_1q_2$ + $ M_2\phi_1q_1^2$ + $ M_3\phi_1q_1q_2$ + $ M_2M_3$ 1.1404 1.2622 0.9035 [X:[1.6102], M:[1.1693, 1.0256, 0.9744], q:[0.3898, 0.441], qb:[], phi:[0.1949]] t^2.34 + t^2.92 + t^3.08 + t^3.23 + t^3.51 + t^3.66 + t^4.09 + t^4.25 + t^4.4 + t^4.68 + t^4.83 + t^5.26 + t^5.42 + t^5.57 + t^5.85 - t^3.58/y - t^4.75/y - t^5.92/y - t^3.58*y - t^4.75*y - t^5.92*y detail