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
1892 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ q_1q_2\tilde{q}_1^2$ 0.6123 0.7911 0.7741 [X:[], M:[0.9708, 1.0877, 1.0292, 0.9123, 0.7135], q:[0.7427, 0.2865], qb:[0.4854, 0.4269], phi:[0.5146]] [X:[], M:[[4], [-12], [-4], [12], [5]], q:[[1], [-5]], qb:[[2], [10]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_5$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ M_4$, $ M_3$, $ \phi_1^2$, $ \phi_1q_2^2$, $ q_1\tilde{q}_2$, $ q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_5^2$, $ M_5q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_5q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ \phi_1q_1q_2$, $ q_2^2\tilde{q}_1^2$, $ M_4M_5$, $ M_4q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_3M_5$, $ M_5\phi_1^2$, $ \phi_1q_1\tilde{q}_1$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_5\phi_1q_2^2$, $ M_3q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_2$, $ M_4^2$, $ M_5q_1\tilde{q}_2$, $ q_1q_2\tilde{q}_2^2$, $ M_3M_4$, $ M_4\phi_1^2$, $ M_5q_1\tilde{q}_1$, $ M_5\phi_1q_2\tilde{q}_2$, $ q_1q_2\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_2^2$ $M_4\phi_1q_2^2$ -1 2*t^2.14 + t^2.32 + t^2.74 + 2*t^3.09 + t^3.26 + t^3.51 + 2*t^3.68 + t^4.11 + 4*t^4.28 + 3*t^4.46 + t^4.63 + 2*t^4.88 + t^5.05 + 4*t^5.23 + 3*t^5.4 + t^5.47 + 2*t^5.65 + 5*t^5.82 - t^6. + 3*t^6.25 + 2*t^6.35 + 7*t^6.42 + t^6.53 + 4*t^6.6 + 4*t^6.77 + t^6.84 + 4*t^7.02 - t^7.12 + 5*t^7.19 + 7*t^7.37 + 3*t^7.54 + 3*t^7.61 + 6*t^7.79 + 7*t^7.97 - 3*t^8.14 + 2*t^8.21 - 2*t^8.32 + 6*t^8.39 + 2*t^8.49 + 12*t^8.56 + t^8.67 + 4*t^8.74 + 4*t^8.91 + 3*t^8.98 - t^4.54/y - t^6.68/y + t^7.28/y + (3*t^7.46)/y - t^7.63/y + (2*t^7.88)/y + t^8.05/y + (4*t^8.23)/y + (5*t^8.4)/y + t^8.58/y + (2*t^8.65)/y + (6*t^8.82)/y - t^4.54*y - t^6.68*y + t^7.28*y + 3*t^7.46*y - t^7.63*y + 2*t^7.88*y + t^8.05*y + 4*t^8.23*y + 5*t^8.4*y + t^8.58*y + 2*t^8.65*y + 6*t^8.82*y 2*g1^5*t^2.14 + t^2.32/g1^3 + g1^12*t^2.74 + (2*t^3.09)/g1^4 + t^3.26/g1^12 + g1^11*t^3.51 + 2*g1^3*t^3.68 + g1^18*t^4.11 + 4*g1^10*t^4.28 + 3*g1^2*t^4.46 + t^4.63/g1^6 + 2*g1^17*t^4.88 + g1^9*t^5.05 + 4*g1*t^5.23 + (3*t^5.4)/g1^7 + g1^24*t^5.47 + 2*g1^16*t^5.65 + 5*g1^8*t^5.82 - t^6. + 3*g1^23*t^6.25 + (2*t^6.35)/g1^16 + 7*g1^15*t^6.42 + t^6.53/g1^24 + 4*g1^7*t^6.6 + (4*t^6.77)/g1 + g1^30*t^6.84 + 4*g1^22*t^7.02 - t^7.12/g1^17 + 5*g1^14*t^7.19 + 7*g1^6*t^7.37 + (3*t^7.54)/g1^2 + 3*g1^29*t^7.61 + 6*g1^21*t^7.79 + 7*g1^13*t^7.97 - 3*g1^5*t^8.14 + 2*g1^36*t^8.21 - (2*t^8.32)/g1^3 + 6*g1^28*t^8.39 + (2*t^8.49)/g1^11 + 12*g1^20*t^8.56 + t^8.67/g1^19 + 4*g1^12*t^8.74 + 4*g1^4*t^8.91 + 3*g1^35*t^8.98 - t^4.54/(g1^2*y) - (g1^3*t^6.68)/y + (g1^10*t^7.28)/y + (3*g1^2*t^7.46)/y - t^7.63/(g1^6*y) + (2*g1^17*t^7.88)/y + (g1^9*t^8.05)/y + (4*g1*t^8.23)/y + (5*t^8.4)/(g1^7*y) + t^8.58/(g1^15*y) + (2*g1^16*t^8.65)/y + (6*g1^8*t^8.82)/y - (t^4.54*y)/g1^2 - g1^3*t^6.68*y + g1^10*t^7.28*y + 3*g1^2*t^7.46*y - (t^7.63*y)/g1^6 + 2*g1^17*t^7.88*y + g1^9*t^8.05*y + 4*g1*t^8.23*y + (5*t^8.4*y)/g1^7 + (t^8.58*y)/g1^15 + 2*g1^16*t^8.65*y + 6*g1^8*t^8.82*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
2914 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ q_1q_2\tilde{q}_1^2$ + $ M_6q_1\tilde{q}_2$ 0.6278 0.8165 0.7689 [X:[], M:[0.9804, 1.0587, 1.0196, 0.9413, 0.7255, 0.8039], q:[0.7451, 0.2745], qb:[0.4902, 0.451], phi:[0.5098]] 2*t^2.18 + t^2.29 + t^2.41 + t^2.82 + 2*t^3.06 + t^3.18 + 2*t^3.71 + t^4.24 + 4*t^4.35 + 3*t^4.47 + 3*t^4.59 + t^4.71 + t^4.82 + 2*t^5. + t^5.12 + 5*t^5.24 + 3*t^5.35 + 2*t^5.47 + t^5.59 + t^5.65 + 4*t^5.88 - t^6. - t^4.53/y - t^4.53*y detail


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
541 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ 0.6135 0.7921 0.7745 [X:[], M:[0.9638, 1.1086, 1.0362, 0.8914, 0.7321], q:[0.7409, 0.2953], qb:[0.4546, 0.4368], phi:[0.5181]] 2*t^2.2 + t^2.25 + t^2.67 + 2*t^3.11 + t^3.33 + t^3.53 + t^3.59 + t^3.75 + t^4.18 + t^4.23 + t^4.28 + 3*t^4.39 + 2*t^4.45 + t^4.5 + 2*t^4.87 + t^4.92 + 4*t^5.3 + t^5.35 + 2*t^5.36 + t^5.52 + 2*t^5.73 + 4*t^5.78 + t^5.84 + t^5.95 - 2*t^6. - t^4.55/y - t^4.55*y detail