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
752 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3\phi_1\tilde{q}_2^2$ + $ M_4q_2\tilde{q}_1$ + $ M_5\phi_1\tilde{q}_1^2$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_1M_6$ 0.6484 0.7959 0.8147 [X:[], M:[0.7035, 1.2965, 0.7108, 0.6962, 0.6962, 1.2965], q:[0.8205, 0.8278], qb:[0.476, 0.4687], phi:[0.3518]] [X:[], M:[[-2, -2], [2, 2], [1, -5], [-5, 1], [-5, 1], [2, 2]], q:[[-1, 2], [2, -1]], qb:[[3, 0], [0, 3]], phi:[[-1, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_4$, $ M_5$, $ M_3$, $ \tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_2$, $ M_2$, $ M_6$, $ q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ M_4M_5$, $ M_5^2$, $ M_3M_4$, $ M_3M_5$, $ M_3^2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_5\tilde{q}_1\tilde{q}_2$, $ q_1q_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_4q_1\tilde{q}_2$, $ M_5q_1\tilde{q}_2$, $ M_2M_4$, $ M_2M_5$, $ M_4M_6$, $ M_5M_6$, $ M_4q_2\tilde{q}_2$, $ M_5q_2\tilde{q}_2$, $ M_4\phi_1\tilde{q}_1\tilde{q}_2$, $ M_5\phi_1\tilde{q}_1\tilde{q}_2$ $M_3q_1\tilde{q}_2$ -4 2*t^2.09 + t^2.13 + t^2.83 + t^3.87 + 4*t^3.89 + 3*t^4.18 + 2*t^4.22 + t^4.26 + 2*t^4.92 + t^4.94 + t^4.97 + t^5.67 + 2*t^5.96 + 6*t^5.98 - 4*t^6. + 2*t^6.02 + 4*t^6.27 + 3*t^6.31 + 2*t^6.35 + t^6.4 + t^6.7 + 4*t^6.72 + 3*t^7.01 - 2*t^7.06 - t^7.08 + t^7.1 + t^7.74 + 4*t^7.76 + 6*t^7.78 - t^7.8 + 3*t^8.05 + 8*t^8.07 - 8*t^8.09 + 3*t^8.11 - 4*t^8.13 + 2*t^8.15 + 5*t^8.35 + 4*t^8.4 + 3*t^8.44 + 2*t^8.49 + t^8.5 + t^8.53 + 2*t^8.79 + 5*t^8.81 - 4*t^8.83 - t^4.06/y - (2*t^6.14)/y - t^6.19/y + t^7.18/y + (2*t^7.22)/y + (3*t^7.92)/y + (3*t^7.97)/y - (3*t^8.23)/y - (2*t^8.28)/y - t^8.32/y + (2*t^8.96)/y + (8*t^8.98)/y - t^4.06*y - 2*t^6.14*y - t^6.19*y + t^7.18*y + 2*t^7.22*y + 3*t^7.92*y + 3*t^7.97*y - 3*t^8.23*y - 2*t^8.28*y - t^8.32*y + 2*t^8.96*y + 8*t^8.98*y (2*g2*t^2.09)/g1^5 + (g1*t^2.13)/g2^5 + g1^3*g2^3*t^2.83 + (g2^5*t^3.87)/g1 + 4*g1^2*g2^2*t^3.89 + (3*g2^2*t^4.18)/g1^10 + (2*t^4.22)/(g1^4*g2^4) + (g1^2*t^4.26)/g2^10 + (2*g2^4*t^4.92)/g1^2 + g1*g2*t^4.94 + (g1^4*t^4.97)/g2^2 + g1^6*g2^6*t^5.67 + (2*g2^6*t^5.96)/g1^6 + (6*g2^3*t^5.98)/g1^3 - 4*t^6. + (2*g1^3*t^6.02)/g2^3 + (4*g2^3*t^6.27)/g1^15 + (3*t^6.31)/(g1^9*g2^3) + (2*t^6.35)/(g1^3*g2^9) + (g1^3*t^6.4)/g2^15 + g1^2*g2^8*t^6.7 + 4*g1^5*g2^5*t^6.72 + (3*g2^5*t^7.01)/g1^7 - (2*t^7.06)/(g1*g2) - (g1^2*t^7.08)/g2^4 + (g1^5*t^7.1)/g2^7 + (g2^10*t^7.74)/g1^2 + 4*g1*g2^7*t^7.76 + 6*g1^4*g2^4*t^7.78 - g1^7*g2*t^7.8 + (3*g2^7*t^8.05)/g1^11 + (8*g2^4*t^8.07)/g1^8 - (8*g2*t^8.09)/g1^5 + (3*t^8.11)/(g1^2*g2^2) - (4*g1*t^8.13)/g2^5 + (2*g1^4*t^8.15)/g2^8 + (5*g2^4*t^8.35)/g1^20 + (4*t^8.4)/(g1^14*g2^2) + (3*t^8.44)/(g1^8*g2^8) + (2*t^8.49)/(g1^2*g2^14) + g1^9*g2^9*t^8.5 + (g1^4*t^8.53)/g2^20 + (2*g2^9*t^8.79)/g1^3 + 5*g2^6*t^8.81 - 4*g1^3*g2^3*t^8.83 - t^4.06/(g1*g2*y) - (2*t^6.14)/(g1^6*y) - t^6.19/(g2^6*y) + (g2^2*t^7.18)/(g1^10*y) + (2*t^7.22)/(g1^4*g2^4*y) + (3*g2^4*t^7.92)/(g1^2*y) + (3*g1^4*t^7.97)/(g2^2*y) - (3*g2*t^8.23)/(g1^11*y) - (2*t^8.28)/(g1^5*g2^5*y) - (g1*t^8.32)/(g2^11*y) + (2*g2^6*t^8.96)/(g1^6*y) + (8*g2^3*t^8.98)/(g1^3*y) - (t^4.06*y)/(g1*g2) - (2*t^6.14*y)/g1^6 - (t^6.19*y)/g2^6 + (g2^2*t^7.18*y)/g1^10 + (2*t^7.22*y)/(g1^4*g2^4) + (3*g2^4*t^7.92*y)/g1^2 + (3*g1^4*t^7.97*y)/g2^2 - (3*g2*t^8.23*y)/g1^11 - (2*t^8.28*y)/(g1^5*g2^5) - (g1*t^8.32*y)/g2^11 + (2*g2^6*t^8.96*y)/g1^6 + (8*g2^3*t^8.98*y)/g1^3


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
1237 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3\phi_1\tilde{q}_2^2$ + $ M_4q_2\tilde{q}_1$ + $ M_5\phi_1\tilde{q}_1^2$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_1M_6$ + $ M_3M_7$ 0.6284 0.7608 0.826 [X:[], M:[0.7147, 1.2853, 0.7375, 0.692, 0.692, 1.2853, 1.2625], q:[0.81, 0.8327], qb:[0.4753, 0.4526], phi:[0.3574]] 2*t^2.08 + t^2.78 + 2*t^3.79 + 4*t^3.86 + 3*t^4.15 + 2*t^4.86 + t^4.93 + t^5.57 + 4*t^5.86 + 6*t^5.93 - 5*t^6. - t^4.07/y - t^4.07*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
457 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3\phi_1\tilde{q}_2^2$ + $ M_4q_2\tilde{q}_1$ + $ M_5\phi_1\tilde{q}_1^2$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ 0.6689 0.835 0.8011 [X:[], M:[0.699, 1.301, 0.7054, 0.6926, 0.6926], q:[0.8221, 0.8284], qb:[0.479, 0.4726], phi:[0.3495]] 2*t^2.08 + t^2.1 + t^2.12 + t^2.85 + t^3.88 + 3*t^3.9 + 3*t^4.16 + 2*t^4.17 + 3*t^4.19 + t^4.21 + t^4.23 + 2*t^4.93 + 2*t^4.95 + t^4.97 + t^5.71 + 2*t^5.96 + 5*t^5.98 - t^6. - t^4.05/y - t^4.05*y detail