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
47891 SU3adj1nf2 $\phi_1^2q_1\tilde{q}_1$ + $ \phi_1^2X_1$ + $ M_1\phi_1q_2\tilde{q}_2$ 1.3396 1.5052 0.8899 [X:[1.4109], M:[0.8836], q:[0.7055, 0.4109], qb:[0.7055, 0.4109], phi:[0.2945]] [X:[[0, 0, 2]], M:[[0, 0, -3]], q:[[-1, 0, 2], [0, -1, 4]], qb:[[1, 0, 0], [0, 1, 0]], phi:[[0, 0, -1]]] 3
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$q_2\tilde{q}_2$, $ M_1$, $ \phi_1^3$, $ q_1\tilde{q}_2$, $ q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ q_1\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_2$, $ X_1$, $ \phi_1q_2\tilde{q}_1$, $ q_2^2\tilde{q}_2^2$, $ \phi_1q_1\tilde{q}_1$, $ M_1q_2\tilde{q}_2$, $ \phi_1^3q_2\tilde{q}_2$, $ M_1^2$, $ M_1\phi_1^3$, $ \phi_1^6$, $ \phi_1\tilde{q}_1\tilde{q}_2^2$, $ \phi_1q_1q_2^2$, $ q_1q_2\tilde{q}_2^2$, $ q_2^2\tilde{q}_1\tilde{q}_2$ $M_1q_2\tilde{q}_1$, $ M_1q_1\tilde{q}_2$ -1 t^2.47 + 2*t^2.65 + 2*t^3.35 + 5*t^4.23 + t^4.93 + 3*t^5.12 + 3*t^5.3 + 2*t^5.47 + 2*t^5.81 - t^6. + 6*t^6.35 + 8*t^6.7 + 3*t^6.88 + t^7.4 + 12*t^7.58 + 2*t^7.77 + 2*t^7.93 + 4*t^7.95 - 4*t^8.12 + 2*t^8.28 + 12*t^8.47 - 2*t^8.65 + 10*t^8.81 + t^8.65/y^2 - t^3.88/y - t^4.77/y - t^6.35/y - (2*t^6.53)/y - (2*t^7.23)/y - (2*t^7.42)/y - t^8.12/y + t^8.3/y + t^8.81/y - t^3.88*y - t^4.77*y - t^6.35*y - 2*t^6.53*y - 2*t^7.23*y - 2*t^7.42*y - t^8.12*y + t^8.3*y + t^8.81*y + t^8.65*y^2 g3^4*t^2.47 + (2*t^2.65)/g3^3 + (g2*g3^2*t^3.35)/g1 + (g1*g3^4*t^3.35)/g2 + (g2*g3*t^4.23)/g1 + 3*g3^2*t^4.23 + (g1*g3^3*t^4.23)/g2 + g3^8*t^4.93 + 3*g3*t^5.12 + (3*t^5.3)/g3^6 + (g1*g2^2*t^5.47)/g3 + (g3^9*t^5.47)/(g1*g2^2) + (g2*g3^6*t^5.81)/g1 + (g1*g3^8*t^5.81)/g2 - 3*t^6. + (g2*t^6.)/(g1*g3) + (g1*g3*t^6.)/g2 + (g2^3*t^6.35)/g3^3 + (g1*g2^2*t^6.35)/g3^2 + (g1^2*g2*t^6.35)/g3 + (g3^7*t^6.35)/(g1^2*g2) + (g3^8*t^6.35)/(g1*g2^2) + (g3^9*t^6.35)/g2^3 + (g2^2*g3^4*t^6.7)/g1^2 + (g2*g3^5*t^6.7)/g1 + 4*g3^6*t^6.7 + (g1*g3^7*t^6.7)/g2 + (g1^2*g3^8*t^6.7)/g2^2 + (3*t^6.88)/g3 + g3^12*t^7.4 + (g2^2*g3^3*t^7.58)/g1^2 + (3*g2*g3^4*t^7.58)/g1 + 4*g3^5*t^7.58 + (3*g1*g3^6*t^7.58)/g2 + (g1^2*g3^7*t^7.58)/g2^2 - (g2*t^7.77)/(g1*g3^3) + (4*t^7.77)/g3^2 - (g1*t^7.77)/(g2*g3) + g1*g2^2*g3^3*t^7.93 + (g3^13*t^7.93)/(g1*g2^2) + (4*t^7.95)/g3^9 - (g2^3*t^8.12)/g3^5 - (g1^2*g2*t^8.12)/g3^3 - (g3^5*t^8.12)/(g1^2*g2) - (g3^7*t^8.12)/g2^3 + (g2*g3^10*t^8.28)/g1 + (g1*g3^12*t^8.28)/g2 + (g2^2*g3^2*t^8.47)/g1^2 + (4*g2*g3^3*t^8.47)/g1 + 2*g3^4*t^8.47 + (4*g1*g3^5*t^8.47)/g2 + (g1^2*g3^6*t^8.47)/g2^2 + (g2*t^8.65)/(g1*g3^4) - (4*t^8.65)/g3^3 + (g1*t^8.65)/(g2*g3^2) + 2*g2^3*g3*t^8.81 + g1*g2^2*g3^2*t^8.81 + 2*g1^2*g2*g3^3*t^8.81 + (2*g3^11*t^8.81)/(g1^2*g2) + (g3^12*t^8.81)/(g1*g2^2) + (2*g3^13*t^8.81)/g2^3 + t^8.65/(g3^3*y^2) - t^3.88/(g3*y) - t^4.77/(g3^2*y) - (g3^3*t^6.35)/y - (2*t^6.53)/(g3^4*y) - (g2*g3*t^7.23)/(g1*y) - (g1*g3^3*t^7.23)/(g2*y) - (2*t^7.42)/(g3^5*y) - (g2*t^8.12)/(g1*y) + (g3*t^8.12)/y - (g1*g3^2*t^8.12)/(g2*y) + t^8.3/(g3^6*y) + (g2*g3^6*t^8.81)/(g1*y) - (g3^7*t^8.81)/y + (g1*g3^8*t^8.81)/(g2*y) - (t^3.88*y)/g3 - (t^4.77*y)/g3^2 - g3^3*t^6.35*y - (2*t^6.53*y)/g3^4 - (g2*g3*t^7.23*y)/g1 - (g1*g3^3*t^7.23*y)/g2 - (2*t^7.42*y)/g3^5 - (g2*t^8.12*y)/g1 + g3*t^8.12*y - (g1*g3^2*t^8.12*y)/g2 + (t^8.3*y)/g3^6 + (g2*g3^6*t^8.81*y)/g1 - g3^7*t^8.81*y + (g1*g3^8*t^8.81*y)/g2 + (t^8.65*y^2)/g3^3


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
47872 SU3adj1nf2 $\phi_1^2q_1\tilde{q}_1$ + $ \phi_1^2X_1$ 1.33 1.4939 0.8903 [X:[1.3964], M:[], q:[0.6982, 0.3964], qb:[0.6982, 0.3964], phi:[0.3018]] t^2.38 + t^2.72 + 3*t^3.28 + 5*t^4.19 + t^4.76 + 2*t^5.09 + 2*t^5.38 + t^5.43 + 3*t^5.66 - 2*t^6. - t^3.91/y - t^4.81/y - t^3.91*y - t^4.81*y detail