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
716 SU2adj1nf2 $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2^2$ + $ M_4\phi_1\tilde{q}_2^2$ + $ M_4M_5$ 0.6496 0.7822 0.8305 [X:[], M:[0.9769, 1.1214, 0.9769, 0.6821, 1.3179], q:[0.7803, 0.4393], qb:[0.5838, 0.4393], phi:[0.4393]] [X:[], M:[[9], [-4], [9], [-6], [6]], q:[[-1], [2]], qb:[[-11], [2]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1^2$, $ M_1$, $ M_3$, $ M_2$, $ q_1q_2$, $ q_1\tilde{q}_2$, $ M_5$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1^4$, $ M_1^2$, $ M_1M_3$, $ M_3^2$ . -4 t^2.64 + 2*t^2.93 + t^3.36 + 2*t^3.66 + 3*t^3.95 + t^4.09 + 2*t^4.39 + t^4.82 + t^5.27 + 3*t^5.86 - 4*t^6. + 2*t^6.29 - 2*t^6.43 + 6*t^6.59 + 4*t^6.88 + 2*t^7.02 + 3*t^7.32 + t^7.46 + 4*t^7.61 + 2*t^7.75 + 6*t^7.91 + 3*t^8.05 + t^8.18 + 2*t^8.34 + 2*t^8.48 - 4*t^8.64 + 2*t^8.77 + 4*t^8.79 + t^8.91 - 8*t^8.93 - t^4.32/y - (2*t^7.25)/y + (2*t^7.39)/y + (2*t^8.57)/y + t^8.86/y - t^4.32*y - 2*t^7.25*y + 2*t^7.39*y + 2*t^8.57*y + t^8.86*y g1^4*t^2.64 + 2*g1^9*t^2.93 + t^3.36/g1^4 + 2*g1*t^3.66 + 3*g1^6*t^3.95 + t^4.09/g1^12 + (2*t^4.39)/g1^7 + t^4.82/g1^20 + g1^8*t^5.27 + 3*g1^18*t^5.86 - 4*t^6. + 2*g1^5*t^6.29 - (2*t^6.43)/g1^13 + 6*g1^10*t^6.59 + 4*g1^15*t^6.88 + (2*t^7.02)/g1^3 + 3*g1^2*t^7.32 + t^7.46/g1^16 + 4*g1^7*t^7.61 + (2*t^7.75)/g1^11 + 6*g1^12*t^7.91 + (3*t^8.05)/g1^6 + t^8.18/g1^24 + (2*t^8.34)/g1 + (2*t^8.48)/g1^19 - 4*g1^4*t^8.64 + (2*t^8.77)/g1^14 + 4*g1^27*t^8.79 + t^8.91/g1^32 - 8*g1^9*t^8.93 - (g1^2*t^4.32)/y - (2*g1^11*t^7.25)/y + (2*t^7.39)/(g1^7*y) + (2*g1^13*t^8.57)/y + (g1^18*t^8.86)/y - g1^2*t^4.32*y - 2*g1^11*t^7.25*y + (2*t^7.39*y)/g1^7 + 2*g1^13*t^8.57*y + g1^18*t^8.86*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
429 SU2adj1nf2 $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2^2$ + $ M_4\phi_1\tilde{q}_2^2$ 0.6704 0.8228 0.8147 [X:[], M:[0.979, 1.1205, 0.979, 0.6807], q:[0.7801, 0.4398], qb:[0.5813, 0.4398], phi:[0.4398]] t^2.04 + t^2.64 + 2*t^2.94 + t^3.36 + 2*t^3.66 + 2*t^3.96 + 2*t^4.08 + 2*t^4.38 + t^4.68 + t^4.81 + 2*t^4.98 + t^5.28 + t^5.4 + 2*t^5.7 + 3*t^5.87 - 2*t^6. - t^4.32/y - t^4.32*y detail