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
8778 Sp2adj1nf1 $\phi_1^2X_1$ + $ q_1^2q_2^2$ + $ \phi_1^4X_2$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1q_1q_2$ + $ M_1M_2$ + $ M_1M_3$ 1.043 1.1367 0.9175 [X:[1.6667, 1.3333], M:[1.1667, 0.8333, 0.8333], q:[0.3333, 0.6667], qb:[], phi:[0.1667]] [X:[[0], [0]], M:[[0], [0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 267/256, c: 291/256, X1: 5/3, X2: 4/3, M1: 7/6, M2: 5/6, M3: 5/6, q1: 1/3, q2: 2/3, phi1: 1/6}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_2$, $ M_3$, $ q_1q_2$, $ \phi_1^3q_1^2$, $ \phi_1^2q_1q_2$, $ X_2$, $ \phi_1^3q_1q_2$, $ \phi_1q_2^2$, $ M_2^2$, $ M_2M_3$, $ M_3^2$, $ X_1$, $ M_2q_1q_2$, $ M_3q_1q_2$, $ \phi_1^3q_2^2$ $M_2\phi_1^3q_1^2$, $ M_3\phi_1^3q_1^2$ 0 2*t^2.5 + t^3. + t^3.5 + 2*t^4. + 2*t^4.5 + 3*t^5. + 2*t^5.5 + 3*t^6.5 + 5*t^7. + 5*t^7.5 + 8*t^8. + t^8.5 + t^8./y^2 - t^3.5/y - t^4.5/y - (2*t^6.)/y - t^6.5/y - (2*t^7.)/y - (2*t^7.5)/y - t^8.5/y - t^3.5*y - t^4.5*y - 2*t^6.*y - t^6.5*y - 2*t^7.*y - 2*t^7.5*y - t^8.5*y + t^8.*y^2 2*t^2.5 + t^3. + t^3.5 + 2*t^4. + 2*t^4.5 + 3*t^5. + 2*t^5.5 + 3*t^6.5 + 5*t^7. + 5*t^7.5 + 8*t^8. + t^8.5 + t^8./y^2 - t^3.5/y - t^4.5/y - (2*t^6.)/y - t^6.5/y - (2*t^7.)/y - (2*t^7.5)/y - t^8.5/y - t^3.5*y - t^4.5*y - 2*t^6.*y - t^6.5*y - 2*t^7.*y - 2*t^7.5*y - t^8.5*y + t^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
8890 $\phi_1^2X_1$ + $ q_1^2q_2^2$ + $ \phi_1^4X_2$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1q_1q_2$ + $ M_1M_2$ + $ M_1M_3$ + $ M_4\phi_1^3q_1^2$ 1.0573 1.1615 0.9103 [X:[1.6667, 1.3333], M:[1.1667, 0.8333, 0.8333, 0.8333], q:[0.3333, 0.6667], qb:[], phi:[0.1667]] 3*t^2.5 + t^3. + 2*t^4. + 2*t^4.5 + 6*t^5. + 3*t^5.5 - 2*t^6. - t^3.5/y - t^4.5/y - (3*t^6.)/y - t^3.5*y - t^4.5*y - 3*t^6.*y detail {a: 203/192, c: 223/192, X1: 5/3, X2: 4/3, M1: 7/6, M2: 5/6, M3: 5/6, M4: 5/6, q1: 1/3, q2: 2/3, phi1: 1/6}


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
8619 Sp2adj1nf1 $\phi_1^2X_1$ + $ q_1^2q_2^2$ + $ \phi_1^4X_2$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1q_1q_2$ + $ M_1M_2$ 1.0286 1.112 0.9251 [X:[1.6667, 1.3333], M:[1.1667, 0.8333], q:[0.3333, 0.6667], qb:[], phi:[0.1667]] t^2.5 + t^3. + 2*t^3.5 + 2*t^4. + 2*t^4.5 + t^5. + t^5.5 - t^3.5/y - t^4.5/y - t^6./y - t^3.5*y - t^4.5*y - t^6.*y detail {a: 395/384, c: 427/384, X1: 5/3, X2: 4/3, M1: 7/6, M2: 5/6, q1: 1/3, q2: 2/3, phi1: 1/6}