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
2771 SU2adj1nf2 $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4q_2\tilde{q}_1$ + $ M_2M_4$ + $ \phi_1q_2^2$ + $ M_3X_1$ + $ M_1M_5$ 0.6173 0.7569 0.8156 [X:[1.4372], M:[0.893, 1.2233, 0.5628, 0.7767, 1.107], q:[0.3302, 0.7767], qb:[0.4465, 0.6605], phi:[0.4465]] [X:[[7]], M:[[-4], [-1], [-7], [1], [4]], q:[[3], [1]], qb:[[-2], [6]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_4$, $ \phi_1^2$, $ q_1\tilde{q}_2$, $ M_5$, $ \phi_1q_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_2$, $ X_1$, $ M_4^2$, $ \phi_1q_1q_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_4q_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_4M_5$, $ M_4\phi_1q_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ q_1^2\tilde{q}_2^2$ $M_5\phi_1^2$, $ \phi_1^3q_1^2$, $ M_4\phi_1q_1\tilde{q}_1$ 1 t^2.33 + t^2.68 + t^2.97 + 3*t^3.32 + 2*t^3.67 + t^4.02 + 2*t^4.31 + 2*t^4.66 + 2*t^5.3 + 3*t^5.65 + t^5.94 + t^6. + 3*t^6.29 - t^6.35 + 6*t^6.64 + 4*t^6.99 + 2*t^7.28 + t^7.34 + 6*t^7.63 + 4*t^7.98 + 2*t^8.04 + 2*t^8.27 - 3*t^8.33 + 6*t^8.62 - 3*t^8.68 + t^8.92 + 3*t^8.97 - t^4.34/y - t^7.02/y + t^7.66/y + t^8.01/y + t^8.3/y + (4*t^8.65)/y - t^4.34*y - t^7.02*y + t^7.66*y + t^8.01*y + t^8.3*y + 4*t^8.65*y g1*t^2.33 + t^2.68/g1^4 + g1^9*t^2.97 + 3*g1^4*t^3.32 + (2*t^3.67)/g1 + t^4.02/g1^6 + 2*g1^7*t^4.31 + 2*g1^2*t^4.66 + 2*g1^10*t^5.3 + 3*g1^5*t^5.65 + g1^18*t^5.94 + t^6. + 3*g1^13*t^6.29 - t^6.35/g1^5 + 6*g1^8*t^6.64 + 4*g1^3*t^6.99 + 2*g1^16*t^7.28 + t^7.34/g1^2 + 6*g1^11*t^7.63 + 4*g1^6*t^7.98 + (2*t^8.04)/g1^12 + 2*g1^19*t^8.27 - 3*g1*t^8.33 + 6*g1^14*t^8.62 - (3*t^8.68)/g1^4 + g1^27*t^8.92 + 3*g1^9*t^8.97 - t^4.34/(g1^2*y) - t^7.02/(g1^6*y) + (g1^2*t^7.66)/y + t^8.01/(g1^3*y) + (g1^10*t^8.3)/y + (4*g1^5*t^8.65)/y - (t^4.34*y)/g1^2 - (t^7.02*y)/g1^6 + g1^2*t^7.66*y + (t^8.01*y)/g1^3 + g1^10*t^8.3*y + 4*g1^5*t^8.65*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
1772 SU2adj1nf2 $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4q_2\tilde{q}_1$ + $ M_2M_4$ + $ \phi_1q_2^2$ + $ M_3X_1$ 0.6277 0.7724 0.8127 [X:[1.4657], M:[0.8767, 1.2192, 0.5343, 0.7808], q:[0.3425, 0.7808], qb:[0.4384, 0.6849], phi:[0.4384]] t^2.34 + 2*t^2.63 + t^3.08 + 2*t^3.37 + 2*t^3.66 + t^3.95 + 2*t^4.4 + 2*t^4.68 + t^4.97 + 2*t^5.26 + 2*t^5.42 + 3*t^5.71 + 2*t^6. - t^4.32/y - t^4.32*y detail