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
46116 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_2\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_2M_4$ 0.5546 0.7066 0.7849 [X:[], M:[0.7599, 1.1364, 0.9672, 0.8636], q:[0.2677, 0.9724], qb:[0.5959, 0.4369], phi:[0.4318]] [X:[], M:[[9, 1], [-2, 2], [-5, -5], [2, -2]], q:[[-3, -2], [-6, 1]], qb:[[5, 0], [0, 5]], phi:[[1, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$q_1\tilde{q}_2$, $ M_1$, $ M_4$, $ \phi_1^2$, $ M_3$, $ \phi_1q_1^2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2\tilde{q}_2$, $ q_1^2\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ q_2\tilde{q}_1$, $ M_4q_1\tilde{q}_2$, $ \phi_1^2q_1\tilde{q}_2$, $ M_1M_4$, $ M_1\phi_1^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1q_2$, $ M_3q_1\tilde{q}_2$, $ \phi_1q_1^3\tilde{q}_2$, $ M_1M_3$, $ M_4^2$, $ M_4\phi_1^2$, $ \phi_1^4$, $ M_3M_4$, $ M_3\phi_1^2$, $ M_4\phi_1q_1^2$, $ \phi_1^3q_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_1^2\tilde{q}_2^2$, $ M_3^2$, $ M_3\phi_1q_1^2$, $ \phi_1^2q_1^4$ $M_4\phi_1q_1\tilde{q}_2$, $ \phi_1^3q_1\tilde{q}_2$ -2 t^2.11 + t^2.28 + 2*t^2.59 + 2*t^2.9 + t^3.41 + t^3.92 + 2*t^4.23 + t^4.39 + t^4.56 + 3*t^4.7 + 2*t^4.87 + 2*t^5.02 + 4*t^5.18 + 3*t^5.49 + t^5.52 + 3*t^5.8 - 2*t^6. + t^6.03 + t^6.2 + 2*t^6.34 - t^6.48 + 2*t^6.51 + t^6.67 - t^6.79 + 4*t^6.82 + t^6.84 + 2*t^6.98 + 3*t^7.13 + 2*t^7.15 + 3*t^7.3 + 4*t^7.46 + 3*t^7.61 + t^7.64 + 5*t^7.77 - 2*t^7.8 + t^7.83 + 3*t^7.92 + 5*t^8.08 - 4*t^8.11 + 2*t^8.14 - 4*t^8.28 + t^8.31 + 4*t^8.39 - t^8.42 + 3*t^8.46 + t^8.48 - 6*t^8.59 + 2*t^8.62 + 4*t^8.71 - t^8.76 + 2*t^8.79 - 8*t^8.9 + 4*t^8.93 + t^8.95 - t^4.3/y - t^6.58/y - t^6.89/y - t^7.2/y + (2*t^7.39)/y + (3*t^7.7)/y + (2*t^7.87)/y + (3*t^8.02)/y + (3*t^8.18)/y + (4*t^8.49)/y + t^8.52/y + t^8.69/y + t^8.8/y - t^8.85/y - t^4.3*y - t^6.58*y - t^6.89*y - t^7.2*y + 2*t^7.39*y + 3*t^7.7*y + 2*t^7.87*y + 3*t^8.02*y + 3*t^8.18*y + 4*t^8.49*y + t^8.52*y + t^8.69*y + t^8.8*y - t^8.85*y (g2^3*t^2.11)/g1^3 + g1^9*g2*t^2.28 + (2*g1^2*t^2.59)/g2^2 + (2*t^2.9)/(g1^5*g2^5) + (g2^2*t^3.41)/g1^2 + g1*g2^9*t^3.92 + (2*g2^6*t^4.23)/g1^6 + g1^6*g2^4*t^4.39 + g1^18*g2^2*t^4.56 + (3*g2*t^4.7)/g1 + (2*g1^11*t^4.87)/g2 + (2*t^5.02)/(g1^8*g2^2) + (4*g1^4*t^5.18)/g2^4 + (3*t^5.49)/(g1^3*g2^7) + (g2^5*t^5.52)/g1^5 + (3*t^5.8)/(g1^10*g2^10) - 2*t^6. + (g2^12*t^6.03)/g1^2 + g1^10*g2^10*t^6.2 + (2*g2^9*t^6.34)/g1^9 - (g1^5*t^6.48)/g2^5 + 2*g1^3*g2^7*t^6.51 + g1^15*g2^5*t^6.67 - t^6.79/(g1^2*g2^8) + (4*g2^4*t^6.82)/g1^4 + g1^27*g2^3*t^6.84 + 2*g1^8*g2^2*t^6.98 + (3*g2*t^7.13)/g1^11 + 2*g1^20*t^7.15 + (3*g1*t^7.3)/g2 + (4*g1^13*t^7.46)/g2^3 + (3*t^7.61)/(g1^6*g2^4) + (g2^8*t^7.64)/g1^8 + (5*g1^6*t^7.77)/g2^6 - 2*g1^4*g2^6*t^7.8 + g1^2*g2^18*t^7.83 + (3*t^7.92)/(g1^13*g2^7) + (5*t^8.08)/(g1*g2^9) - (4*g2^3*t^8.11)/g1^3 + (2*g2^15*t^8.14)/g1^5 - 4*g1^9*g2*t^8.28 + g1^7*g2^13*t^8.31 + (4*t^8.39)/(g1^8*g2^12) - t^8.42/g1^10 + (3*g2^12*t^8.46)/g1^12 + g1^19*g2^11*t^8.48 - (6*g1^2*t^8.59)/g2^2 + 2*g2^10*t^8.62 + (4*t^8.71)/(g1^15*g2^15) - (g1^14*t^8.76)/g2^4 + 2*g1^12*g2^8*t^8.79 - (8*t^8.9)/(g1^5*g2^5) + (4*g2^7*t^8.93)/g1^7 + g1^24*g2^6*t^8.95 - (g1*t^4.3)/(g2*y) - (g1^10*t^6.58)/y - (g1^3*t^6.89)/(g2^3*y) - t^7.2/(g1^4*g2^6*y) + (2*g1^6*g2^4*t^7.39)/y + (3*g2*t^7.7)/(g1*y) + (2*g1^11*t^7.87)/(g2*y) + (3*t^8.02)/(g1^8*g2^2*y) + (3*g1^4*t^8.18)/(g2^4*y) + (4*t^8.49)/(g1^3*g2^7*y) + (g2^5*t^8.52)/(g1^5*y) + (g1^7*g2^3*t^8.69)/y + t^8.8/(g1^10*g2^10*y) - (g1^19*g2*t^8.85)/y - (g1*t^4.3*y)/g2 - g1^10*t^6.58*y - (g1^3*t^6.89*y)/g2^3 - (t^7.2*y)/(g1^4*g2^6) + 2*g1^6*g2^4*t^7.39*y + (3*g2*t^7.7*y)/g1 + (2*g1^11*t^7.87*y)/g2 + (3*t^8.02*y)/(g1^8*g2^2) + (3*g1^4*t^8.18*y)/g2^4 + (4*t^8.49*y)/(g1^3*g2^7) + (g2^5*t^8.52*y)/g1^5 + g1^7*g2^3*t^8.69*y + (t^8.8*y)/(g1^10*g2^10) - g1^19*g2*t^8.85*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
45970 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_2\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ 0.5429 0.6874 0.7898 [X:[], M:[0.7766, 1.1258, 0.9719], q:[0.2674, 0.9561], qb:[0.6068, 0.4213], phi:[0.4371]] t^2.07 + t^2.33 + t^2.62 + 2*t^2.92 + 2*t^3.38 + t^3.84 + 2*t^4.13 + t^4.4 + t^4.66 + 2*t^4.69 + t^4.95 + 2*t^4.98 + 2*t^5.25 + 2*t^5.44 + t^5.54 + t^5.71 + 3*t^5.83 + t^5.9 - 2*t^6. - t^4.31/y - t^4.31*y detail