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
8349 G2adj1nf1 $\phi_1^2X_1$ + $ \phi_1^9q_1$ + $ q_1^2X_2$ + $ M_1\phi_1^4q_1^2$ + $ M_2\phi_1^6$ 1.218 1.343 0.9069 [X:[1.6, 1.6], M:[0.8, 0.8], q:[0.2], qb:[], phi:[0.2]] [X:[[0], [0]], M:[[0], [0]], q:[[0]], qb:[], phi:[[0]]] 0 {a: 609/500, c: 1343/1000, X1: 8/5, X2: 8/5, M1: 4/5, M2: 4/5, q1: 1/5, phi1: 1/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ M_2$, $ \phi_1^3q_1$, $ \phi_1^2q_1^2$, $ \phi_1^3q_1^3$, $ M_1^2$, $ M_1M_2$, $ M_2^2$, $ M_1\phi_1^3q_1$, $ M_2\phi_1^3q_1$, $ M_1\phi_1^2q_1^2$, $ M_2\phi_1^2q_1^2$, $ \phi_1^6q_1^2$, $ \phi_1^5q_1^3$, $ \phi_1^4q_1^4$, $ X_1$, $ X_2$, $ \phi_1^6q_1^3$ $M_1\phi_1^3q_1^3$, $ M_2\phi_1^3q_1^3$, $ \phi_1^6q_1^4$, $ \phi_1^5q_1^5$ 3 4*t^2.4 + t^3.6 + 12*t^4.8 + t^5.4 + 3*t^6. + 26*t^7.2 + t^7.8 + 5*t^8.4 + t^8.4/y^2 - t^3.6/y - t^4.8/y - (5*t^6.)/y - (3*t^7.2)/y + (6*t^7.8)/y - (12*t^8.4)/y - t^3.6*y - t^4.8*y - 5*t^6.*y - 3*t^7.2*y + 6*t^7.8*y - 12*t^8.4*y + t^8.4*y^2 4*t^2.4 + t^3.6 + 12*t^4.8 + t^5.4 + 3*t^6. + 26*t^7.2 + t^7.8 + 5*t^8.4 + t^8.4/y^2 - t^3.6/y - t^4.8/y - (5*t^6.)/y - (3*t^7.2)/y + (6*t^7.8)/y - (12*t^8.4)/y - t^3.6*y - t^4.8*y - 5*t^6.*y - 3*t^7.2*y + 6*t^7.8*y - 12*t^8.4*y + t^8.4*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
8902 $\phi_1^2X_1$ + $ \phi_1^9q_1$ + $ q_1^2X_2$ + $ M_1\phi_1^4q_1^2$ + $ M_2\phi_1^6$ + $ M_3\phi_1^3q_1^3$ 1.2345 1.372 0.8998 [X:[1.6, 1.6], M:[0.8, 0.8, 0.8], q:[0.2], qb:[], phi:[0.2]] 5*t^2.4 + 17*t^4.8 + t^5.4 - t^6. - t^3.6/y - t^4.8/y - (6*t^6.)/y - t^3.6*y - t^4.8*y - 6*t^6.*y detail {a: 2469/2000, c: 343/250, X1: 8/5, X2: 8/5, M1: 4/5, M2: 4/5, M3: 4/5, q1: 1/5, phi1: 1/5}


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
8329 G2adj1nf1 $\phi_1^2X_1$ + $ \phi_1^9q_1$ + $ q_1^2X_2$ + $ M_1\phi_1^4q_1^2$ 1.2015 1.314 0.9144 [X:[1.6, 1.6], M:[0.8], q:[0.2], qb:[], phi:[0.2]] 3*t^2.4 + 2*t^3.6 + 8*t^4.8 + t^5.4 + 5*t^6. - t^3.6/y - t^4.8/y - (4*t^6.)/y - t^3.6*y - t^4.8*y - 4*t^6.*y detail {a: 2403/2000, c: 657/500, X1: 8/5, X2: 8/5, M1: 4/5, q1: 1/5, phi1: 1/5}