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
56978 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1^2$ + $ M_6\phi_1q_1^2$ + $ M_7\phi_1q_2^2$ + $ M_7q_2\tilde{q}_1$ 0.647 0.8101 0.7986 [X:[], M:[1.2057, 0.8014, 0.7943, 0.8157, 1.1914, 0.78, 0.8229], q:[0.4079, 0.3864], qb:[0.7907, 0.7979], phi:[0.4043]] [X:[], M:[[-8], [-2], [8], [-22], [12], [28], [-32]], q:[[-11], [19]], qb:[[13], [3]], phi:[[-6]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_6$, $ M_3$, $ M_2$, $ M_4$, $ M_7$, $ q_2\tilde{q}_1$, $ M_5$, $ \phi_1q_1q_2$, $ M_1$, $ M_6^2$, $ M_3M_6$, $ M_2M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_3^2$, $ \phi_1q_2\tilde{q}_2$, $ \tilde{q}_1\tilde{q}_2$, $ M_2M_3$, $ M_4M_6$, $ M_2^2$, $ M_6M_7$, $ \phi_1q_1\tilde{q}_1$, $ M_3M_4$, $ \phi_1q_1\tilde{q}_2$, $ M_2M_4$, $ M_3M_7$, $ M_2M_7$, $ M_4^2$, $ M_4M_7$, $ M_7^2$, $ M_6q_2\tilde{q}_1$, $ M_5M_6$, $ M_3q_2\tilde{q}_1$, $ M_6\phi_1q_1q_2$, $ M_2q_2\tilde{q}_1$, $ M_3M_5$, $ M_1M_6$, $ \phi_1\tilde{q}_1^2$, $ M_2M_5$, $ M_4q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$ . -1 t^2.34 + t^2.38 + t^2.4 + t^2.45 + t^2.47 + t^3.53 + t^3.57 + t^3.6 + t^3.62 + t^4.68 + t^4.72 + 2*t^4.74 + 2*t^4.77 + t^4.79 + 3*t^4.81 + t^4.83 + t^4.85 + t^4.87 + t^4.89 + t^4.92 + t^4.94 + t^5.87 + 2*t^5.91 + t^5.94 + 3*t^5.96 + 2*t^5.98 - t^6. + t^6.02 + t^6.04 + t^6.09 + t^7.02 + 2*t^7.06 + 2*t^7.08 + 2*t^7.11 + 2*t^7.13 + 4*t^7.15 + t^7.17 + 2*t^7.19 + 3*t^7.21 + t^7.23 + 3*t^7.26 + 3*t^7.28 + t^7.3 + t^7.32 + 2*t^7.34 + t^7.36 + t^7.38 + t^7.41 + t^8.21 + 2*t^8.25 + 2*t^8.28 + 4*t^8.3 + t^8.32 + t^8.34 + 2*t^8.36 - t^8.4 + 2*t^8.43 - 2*t^8.45 - 2*t^8.47 + t^8.49 + t^8.55 - t^4.21/y - t^6.55/y - t^6.62/y - t^6.66/y - t^6.68/y + t^7.72/y + (2*t^7.74)/y + t^7.77/y + (2*t^7.79)/y + (2*t^7.81)/y + t^7.83/y + (2*t^7.85)/y + (2*t^7.87)/y + t^7.92/y + t^8.87/y - t^8.89/y + (2*t^8.91)/y + (2*t^8.94)/y + t^8.96/y + (3*t^8.98)/y - t^4.21*y - t^6.55*y - t^6.62*y - t^6.66*y - t^6.68*y + t^7.72*y + 2*t^7.74*y + t^7.77*y + 2*t^7.79*y + 2*t^7.81*y + t^7.83*y + 2*t^7.85*y + 2*t^7.87*y + t^7.92*y + t^8.87*y - t^8.89*y + 2*t^8.91*y + 2*t^8.94*y + t^8.96*y + 3*t^8.98*y g1^28*t^2.34 + g1^8*t^2.38 + t^2.4/g1^2 + t^2.45/g1^22 + t^2.47/g1^32 + g1^32*t^3.53 + g1^12*t^3.57 + g1^2*t^3.6 + t^3.62/g1^8 + g1^56*t^4.68 + g1^36*t^4.72 + 2*g1^26*t^4.74 + 2*g1^16*t^4.77 + g1^6*t^4.79 + (3*t^4.81)/g1^4 + t^4.83/g1^14 + t^4.85/g1^24 + t^4.87/g1^34 + t^4.89/g1^44 + t^4.92/g1^54 + t^4.94/g1^64 + g1^60*t^5.87 + 2*g1^40*t^5.91 + g1^30*t^5.94 + 3*g1^20*t^5.96 + 2*g1^10*t^5.98 - t^6. + t^6.02/g1^10 + t^6.04/g1^20 + t^6.09/g1^40 + g1^84*t^7.02 + 2*g1^64*t^7.06 + 2*g1^54*t^7.08 + 2*g1^44*t^7.11 + 2*g1^34*t^7.13 + 4*g1^24*t^7.15 + g1^14*t^7.17 + 2*g1^4*t^7.19 + (3*t^7.21)/g1^6 + t^7.23/g1^16 + (3*t^7.26)/g1^26 + (3*t^7.28)/g1^36 + t^7.3/g1^46 + t^7.32/g1^56 + (2*t^7.34)/g1^66 + t^7.36/g1^76 + t^7.38/g1^86 + t^7.41/g1^96 + g1^88*t^8.21 + 2*g1^68*t^8.25 + 2*g1^58*t^8.28 + 4*g1^48*t^8.3 + g1^38*t^8.32 + g1^28*t^8.34 + 2*g1^18*t^8.36 - t^8.4/g1^2 + (2*t^8.43)/g1^12 - (2*t^8.45)/g1^22 - (2*t^8.47)/g1^32 + t^8.49/g1^42 + t^8.55/g1^72 - t^4.21/(g1^6*y) - (g1^22*t^6.55)/y - t^6.62/(g1^8*y) - t^6.66/(g1^28*y) - t^6.68/(g1^38*y) + (g1^36*t^7.72)/y + (2*g1^26*t^7.74)/y + (g1^16*t^7.77)/y + (2*g1^6*t^7.79)/y + (2*t^7.81)/(g1^4*y) + t^7.83/(g1^14*y) + (2*t^7.85)/(g1^24*y) + (2*t^7.87)/(g1^34*y) + t^7.92/(g1^54*y) + (g1^60*t^8.87)/y - (g1^50*t^8.89)/y + (2*g1^40*t^8.91)/y + (2*g1^30*t^8.94)/y + (g1^20*t^8.96)/y + (3*g1^10*t^8.98)/y - (t^4.21*y)/g1^6 - g1^22*t^6.55*y - (t^6.62*y)/g1^8 - (t^6.66*y)/g1^28 - (t^6.68*y)/g1^38 + g1^36*t^7.72*y + 2*g1^26*t^7.74*y + g1^16*t^7.77*y + 2*g1^6*t^7.79*y + (2*t^7.81*y)/g1^4 + (t^7.83*y)/g1^14 + (2*t^7.85*y)/g1^24 + (2*t^7.87*y)/g1^34 + (t^7.92*y)/g1^54 + g1^60*t^8.87*y - g1^50*t^8.89*y + 2*g1^40*t^8.91*y + 2*g1^30*t^8.94*y + g1^20*t^8.96*y + 3*g1^10*t^8.98*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
55354 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1^2$ + $ M_6\phi_1q_1^2$ + $ M_7\phi_1q_2^2$ 0.6918 0.8766 0.7892 [X:[], M:[1.1677, 1.0397, 0.8323, 0.7938, 1.0833, 0.7479, 0.6708], q:[0.3969, 0.4354], qb:[0.5634, 0.7708], phi:[0.4584]] t^2.01 + t^2.24 + t^2.38 + t^2.5 + t^3. + t^3.12 + t^3.25 + t^3.5 + t^3.87 + t^4. + t^4.02 + 2*t^4.26 + t^4.37 + t^4.39 + t^4.49 + t^4.51 + t^4.62 + t^4.74 + 2*t^4.76 + t^4.88 + t^4.99 + t^5.01 + t^5.13 + t^5.24 + t^5.26 + t^5.36 + t^5.38 + 2*t^5.49 + t^5.52 + t^5.63 + 2*t^5.75 + t^5.88 + t^5.99 - 2*t^6. - t^4.38/y - t^4.38*y detail