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
47148 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_1M_3$ + $ \phi_1q_1^2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_2M_5$ 0.6152 0.7517 0.8185 [X:[], M:[0.8167, 0.761, 1.1833, 0.7888, 1.239], q:[0.8028, 0.3805], qb:[0.4363, 0.8028], phi:[0.3944]] [X:[], M:[[6], [-14], [-6], [-4], [14]], q:[[1], [-7]], qb:[[13], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_4$, $ \phi_1^2$, $ M_1$, $ \phi_1q_2^2$, $ M_3$, $ q_2\tilde{q}_2$, $ M_5$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ M_4^2$, $ M_4\phi_1^2$, $ \phi_1^4$, $ \phi_1q_1q_2$, $ M_1M_4$, $ M_1\phi_1^2$, $ q_1\tilde{q}_2$, $ M_1^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4\phi_1q_2^2$, $ \phi_1^3q_2^2$, $ M_3M_4$, $ M_3\phi_1^2$, $ M_4q_2\tilde{q}_2$ . -1 2*t^2.37 + t^2.45 + t^3.47 + 2*t^3.55 + 2*t^3.72 + t^3.8 + 3*t^4.73 + 3*t^4.82 + t^4.9 + t^5.83 + 3*t^5.92 - t^6. + 2*t^6.08 + 3*t^6.17 + t^6.25 + t^6.93 + t^7.02 + 4*t^7.1 + 3*t^7.18 + 3*t^7.27 + 2*t^7.43 + 2*t^7.52 + t^7.6 + t^8.2 + 3*t^8.28 - 2*t^8.37 - t^8.45 + 3*t^8.53 + 3*t^8.62 + t^8.7 - t^4.18/y - (2*t^6.55)/y + t^7.73/y + (4*t^7.82)/y + (2*t^8.83)/y + (2*t^8.92)/y - t^4.18*y - 2*t^6.55*y + t^7.73*y + 4*t^7.82*y + 2*t^8.83*y + 2*t^8.92*y (2*t^2.37)/g1^4 + g1^6*t^2.45 + t^3.47/g1^16 + (2*t^3.55)/g1^6 + 2*g1^14*t^3.72 + g1^24*t^3.8 + (3*t^4.73)/g1^8 + 3*g1^2*t^4.82 + g1^12*t^4.9 + t^5.83/g1^20 + (3*t^5.92)/g1^10 - t^6. + 2*g1^10*t^6.08 + 3*g1^20*t^6.17 + g1^30*t^6.25 + t^6.93/g1^32 + t^7.02/g1^22 + (4*t^7.1)/g1^12 + (3*t^7.18)/g1^2 + 3*g1^8*t^7.27 + 2*g1^28*t^7.43 + 2*g1^38*t^7.52 + g1^48*t^7.6 + t^8.2/g1^24 + (3*t^8.28)/g1^14 - (2*t^8.37)/g1^4 - g1^6*t^8.45 + 3*g1^16*t^8.53 + 3*g1^26*t^8.62 + g1^36*t^8.7 - t^4.18/(g1^2*y) - (2*t^6.55)/(g1^6*y) + t^7.73/(g1^8*y) + (4*g1^2*t^7.82)/y + (2*t^8.83)/(g1^20*y) + (2*t^8.92)/(g1^10*y) - (t^4.18*y)/g1^2 - (2*t^6.55*y)/g1^6 + (t^7.73*y)/g1^8 + 4*g1^2*t^7.82*y + (2*t^8.83*y)/g1^20 + (2*t^8.92*y)/g1^10


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
46647 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_1M_3$ + $ \phi_1q_1^2$ + $ M_4\phi_1q_2\tilde{q}_1$ 0.6342 0.7862 0.8067 [X:[], M:[0.8241, 0.7438, 1.1759, 0.784], q:[0.804, 0.3719], qb:[0.4521, 0.804], phi:[0.392]] t^2.23 + 2*t^2.35 + t^2.47 + t^3.41 + 2*t^3.53 + t^3.77 + t^3.89 + t^4.46 + 2*t^4.58 + 4*t^4.7 + 3*t^4.82 + t^4.94 + t^5.64 + 3*t^5.76 + 3*t^5.88 - t^4.18/y - t^4.18*y detail