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
3768 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_1$ + $ M_2M_5$ + $ M_6q_1\tilde{q}_2$ + $ M_5M_7$ 0.6226 0.8101 0.7686 [X:[], M:[0.9519, 1.1442, 0.9519, 0.7597, 0.8558, 0.8123, 1.1442], q:[0.738, 0.3101], qb:[0.4062, 0.4497], phi:[0.524]] [X:[], M:[[4], [-12], [4], [20], [12], [-26], [-12]], q:[[1], [-5]], qb:[[-13], [25]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$q_2\tilde{q}_1$, $ M_4$, $ q_2\tilde{q}_2$, $ M_6$, $ M_1$, $ M_3$, $ M_2$, $ M_7$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_1^2$, $ M_4q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ M_4q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_6q_2\tilde{q}_1$, $ M_4M_6$, $ \phi_1q_1q_2$, $ M_6q_2\tilde{q}_2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ M_3q_2\tilde{q}_1$, $ M_1M_4$, $ M_3M_4$, $ \phi_1q_1\tilde{q}_2$, $ M_3q_2\tilde{q}_2$, $ M_1M_6$, $ M_3M_6$, $ M_7q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_1^2$, $ M_1M_3$, $ M_3^2$, $ M_2M_4$, $ M_4M_7$, $ M_4\phi_1q_2^2$, $ M_7q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_2M_6$, $ M_6M_7$, $ M_6\phi_1q_2^2$ . -3 t^2.15 + 2*t^2.28 + t^2.44 + 2*t^2.86 + 3*t^3.43 + t^3.85 + t^4.01 + t^4.14 + t^4.27 + t^4.3 + 2*t^4.43 + 3*t^4.56 + t^4.59 + 2*t^4.72 + t^4.87 + 2*t^5. + 4*t^5.14 + 2*t^5.29 + 2*t^5.58 + 7*t^5.71 + 2*t^5.87 - 3*t^6. + t^6.13 + t^6.16 + 6*t^6.29 + t^6.42 + 2*t^6.45 + 2*t^6.55 + t^6.58 + 4*t^6.71 + t^6.73 + 4*t^6.84 + 7*t^6.86 + 2*t^7. + t^7.02 + t^7.13 + 2*t^7.15 + 3*t^7.28 + t^7.31 + 5*t^7.41 + 3*t^7.44 + 2*t^7.57 + t^7.7 + 4*t^7.73 + 3*t^7.86 + 9*t^7.99 + 2*t^8.02 + t^8.12 + 3*t^8.15 - 6*t^8.28 + 3*t^8.31 + 2*t^8.41 + t^8.54 + 9*t^8.57 + 2*t^8.59 + t^8.7 + 4*t^8.73 + 3*t^8.83 - 7*t^8.86 + 2*t^8.88 + 4*t^8.99 - t^4.57/y - t^6.85/y - t^7.01/y + t^7.14/y + t^7.43/y + t^7.56/y + t^7.59/y + (3*t^7.72)/y + t^8./y + (5*t^8.14)/y + (3*t^8.29)/y + (3*t^8.58)/y + (7*t^8.71)/y + (3*t^8.87)/y - t^4.57*y - t^6.85*y - t^7.01*y + t^7.14*y + t^7.43*y + t^7.56*y + t^7.59*y + 3*t^7.72*y + t^8.*y + 5*t^8.14*y + 3*t^8.29*y + 3*t^8.58*y + 7*t^8.71*y + 3*t^8.87*y t^2.15/g1^18 + 2*g1^20*t^2.28 + t^2.44/g1^26 + 2*g1^4*t^2.86 + (3*t^3.43)/g1^12 + g1^18*t^3.85 + t^4.01/g1^28 + g1^10*t^4.14 + g1^48*t^4.27 + t^4.3/g1^36 + 2*g1^2*t^4.43 + 3*g1^40*t^4.56 + t^4.59/g1^44 + (2*t^4.72)/g1^6 + t^4.87/g1^52 + (2*t^5.)/g1^14 + 4*g1^24*t^5.14 + (2*t^5.29)/g1^22 + (2*t^5.58)/g1^30 + 7*g1^8*t^5.71 + (2*t^5.87)/g1^38 - 3*t^6. + g1^38*t^6.13 + t^6.16/g1^46 + (6*t^6.29)/g1^8 + g1^30*t^6.42 + (2*t^6.45)/g1^54 + 2*g1^68*t^6.55 + t^6.58/g1^16 + 4*g1^22*t^6.71 + t^6.73/g1^62 + 4*g1^60*t^6.84 + (7*t^6.86)/g1^24 + 2*g1^14*t^7. + t^7.02/g1^70 + g1^52*t^7.13 + (2*t^7.15)/g1^32 + 3*g1^6*t^7.28 + t^7.31/g1^78 + 5*g1^44*t^7.41 + (3*t^7.44)/g1^40 + (2*t^7.57)/g1^2 + g1^36*t^7.7 + (4*t^7.73)/g1^48 + (3*t^7.86)/g1^10 + 9*g1^28*t^7.99 + (2*t^8.02)/g1^56 + g1^66*t^8.12 + (3*t^8.15)/g1^18 - 6*g1^20*t^8.28 + (3*t^8.31)/g1^64 + 2*g1^58*t^8.41 + g1^96*t^8.54 + 9*g1^12*t^8.57 + (2*t^8.59)/g1^72 + g1^50*t^8.7 + (4*t^8.73)/g1^34 + 3*g1^88*t^8.83 - 7*g1^4*t^8.86 + (2*t^8.88)/g1^80 + 4*g1^42*t^8.99 - t^4.57/(g1^2*y) - (g1^18*t^6.85)/y - t^7.01/(g1^28*y) + (g1^10*t^7.14)/y + (g1^2*t^7.43)/y + (g1^40*t^7.56)/y + t^7.59/(g1^44*y) + (3*t^7.72)/(g1^6*y) + t^8./(g1^14*y) + (5*g1^24*t^8.14)/y + (3*t^8.29)/(g1^22*y) + (3*t^8.58)/(g1^30*y) + (7*g1^8*t^8.71)/y + (3*t^8.87)/(g1^38*y) - (t^4.57*y)/g1^2 - g1^18*t^6.85*y - (t^7.01*y)/g1^28 + g1^10*t^7.14*y + g1^2*t^7.43*y + g1^40*t^7.56*y + (t^7.59*y)/g1^44 + (3*t^7.72*y)/g1^6 + (t^8.*y)/g1^14 + 5*g1^24*t^8.14*y + (3*t^8.29*y)/g1^22 + (3*t^8.58*y)/g1^30 + 7*g1^8*t^8.71*y + (3*t^8.87*y)/g1^38


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
3327 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_1$ + $ M_2M_5$ + $ M_6q_1\tilde{q}_2$ 0.6355 0.8324 0.7635 [X:[], M:[0.9501, 1.1498, 0.9501, 0.7504, 0.8502, 0.8245], q:[0.7375, 0.3124], qb:[0.4123, 0.438], phi:[0.525]] t^2.17 + 2*t^2.25 + t^2.47 + t^2.55 + 2*t^2.85 + 2*t^3.45 + t^3.83 + t^4.05 + t^4.13 + t^4.2 + t^4.35 + 2*t^4.43 + 3*t^4.5 + t^4.65 + 3*t^4.72 + 2*t^4.8 + t^4.95 + 3*t^5.02 + 5*t^5.1 + 2*t^5.32 + 2*t^5.4 + t^5.62 + 5*t^5.7 + t^5.92 - t^6. - t^4.57/y - t^4.57*y detail