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
199 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_1\phi_1^2$ + $ q_1\tilde{q}_1\tilde{q}_2^2$ + $ M_2X_1$ 0.4728 0.5871 0.8053 [X:[1.5958], M:[1.1917, 0.4042], q:[0.6167, 0.9791], qb:[0.1917, 0.5958], phi:[0.4042]] [X:[[1]], M:[[2], [-1]], q:[[-4], [5]], qb:[[2], [1]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1\tilde{q}_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1^2$, $ q_2\tilde{q}_1$, $ M_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_2$, $ \phi_1^2\tilde{q}_1^4$, $ q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^3\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ q_1q_2$, $ \phi_1^3\tilde{q}_1^2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ X_1$, $ \phi_1q_2\tilde{q}_1^3$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_1\phi_1\tilde{q}_1^2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ \phi_1^2\tilde{q}_1^3\tilde{q}_2$, $ \phi_1\tilde{q}_1^2\tilde{q}_2^2$ $\phi_1^3\tilde{q}_1\tilde{q}_2$ -1 2*t^2.36 + t^2.43 + t^3.51 + 2*t^3.57 + t^3.64 + 4*t^4.72 + 3*t^4.79 + 2*t^5.87 + 3*t^5.94 - t^6. - t^6.06 + t^7.02 + 7*t^7.09 + 4*t^7.15 - 2*t^7.21 + 4*t^8.24 + 5*t^8.3 - 4*t^8.36 - 3*t^8.43 - t^8.49 - t^4.21/y + t^7.72/y + (2*t^7.79)/y + (2*t^8.87)/y + (5*t^8.94)/y - t^4.21*y + t^7.72*y + 2*t^7.79*y + 2*t^8.87*y + 5*t^8.94*y 2*g1^3*t^2.36 + t^2.43/g1^2 + g1^7*t^3.51 + 2*g1^2*t^3.57 + t^3.64/g1^3 + 4*g1^6*t^4.72 + 3*g1*t^4.79 + 2*g1^10*t^5.87 + 3*g1^5*t^5.94 - t^6. - t^6.06/g1^5 + g1^14*t^7.02 + 7*g1^9*t^7.09 + 4*g1^4*t^7.15 - (2*t^7.21)/g1 + 4*g1^13*t^8.24 + 5*g1^8*t^8.3 - 4*g1^3*t^8.36 - (3*t^8.43)/g1^2 - t^8.49/g1^7 - t^4.21/(g1*y) + (g1^6*t^7.72)/y + (2*g1*t^7.79)/y + (2*g1^10*t^8.87)/y + (5*g1^5*t^8.94)/y - (t^4.21*y)/g1 + g1^6*t^7.72*y + 2*g1*t^7.79*y + 2*g1^10*t^8.87*y + 5*g1^5*t^8.94*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
121 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_1\phi_1^2$ 0.5427 0.6891 0.7875 [X:[], M:[1.1204, 0.7357], q:[0.6112, 0.949], qb:[0.2684, 0.4122], phi:[0.4398]] t^2.04 + t^2.21 + t^2.64 + t^2.93 + t^3.07 + 2*t^3.36 + t^3.65 + 2*t^4.08 + t^4.25 + t^4.41 + 2*t^4.68 + t^4.85 + t^4.97 + t^5.11 + t^5.14 + t^5.28 + 2*t^5.4 + 2*t^5.57 + t^5.69 + 2*t^5.86 - t^6. - t^4.32/y - t^4.32*y detail