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
45127 SO5adj1nf2 $\phi_1^4q_1$ + $ q_1^4$ + $ M_1q_1q_2$ + $ M_2\phi_1^2$ 1.7523 1.8461 0.9492 [X:[], M:[1.125, 1.25], q:[0.5, 0.375], qb:[], phi:[0.375]] [X:[], M:[[0], [0]], q:[[0], [0]], qb:[], phi:[[0]]] 0 {a: 14355/8192, c: 15123/8192, M1: 9/8, M2: 5/4, q1: 1/2, q2: 3/8, phi1: 3/8}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$q_2^2$, $ q_1^2$, $ M_1$, $ \phi_1^2q_2$, $ M_2$, $ \phi_1^2q_1$, $ \phi_1q_1q_2$, $ \phi_1^4$, $ \phi_1^2q_2^2$, $ q_2^4$, $ \phi_1^2q_1q_2$, $ \phi_1^2q_1^2$, $ q_1^2q_2^2$, $ M_1q_2^2$, $ \phi_1^2q_2^3$ $\phi_1^3q_1q_2$, $ M_2q_2^2$, $ \phi_1^2q_1q_2^2$, $ \phi_1q_1q_2^3$ 3 t^2.25 + t^3. + 2*t^3.38 + 3*t^3.75 + 3*t^4.5 + t^4.88 + 2*t^5.25 + t^5.62 + 3*t^6. + t^6.38 + 7*t^6.75 + 5*t^7.12 + 8*t^7.5 + 5*t^7.88 + 9*t^8.25 + 2*t^8.62 - t^4.12/y - t^5.25/y - t^5.62/y - (2*t^6.38)/y - t^7.12/y - (3*t^7.5)/y - (3*t^7.88)/y - (3*t^8.62)/y - t^4.12*y - t^5.25*y - t^5.62*y - 2*t^6.38*y - t^7.12*y - 3*t^7.5*y - 3*t^7.88*y - 3*t^8.62*y t^2.25 + t^3. + 2*t^3.38 + 3*t^3.75 + 3*t^4.5 + t^4.88 + 2*t^5.25 + t^5.62 + 3*t^6. + t^6.38 + 7*t^6.75 + 5*t^7.12 + 8*t^7.5 + 5*t^7.88 + 9*t^8.25 + 2*t^8.62 - t^4.12/y - t^5.25/y - t^5.62/y - (2*t^6.38)/y - t^7.12/y - (3*t^7.5)/y - (3*t^7.88)/y - (3*t^8.62)/y - t^4.12*y - t^5.25*y - t^5.62*y - 2*t^6.38*y - t^7.12*y - 3*t^7.5*y - 3*t^7.88*y - 3*t^8.62*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


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
45019 SO5adj1nf2 $\phi_1^4q_1$ + $ q_1^4$ + $ M_1q_1q_2$ 1.7714 1.8807 0.9418 [X:[], M:[1.125], q:[0.5, 0.375], qb:[], phi:[0.375]] 2*t^2.25 + t^3. + 2*t^3.38 + 2*t^3.75 + 5*t^4.5 + t^4.88 + 3*t^5.25 + 3*t^5.62 + 4*t^6. - t^4.12/y - t^5.25/y - t^5.62/y - t^4.12*y - t^5.25*y - t^5.62*y detail {a: 14511/8192, c: 15407/8192, M1: 9/8, q1: 1/2, q2: 3/8, phi1: 3/8}