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
32 SU2adj1nf1 $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_3\phi_1q_1\tilde{q}_1$ + $ M_1M_3$ + $ M_1M_4$ 0.4419 0.5359 0.8246 [X:[1.4016], M:[1.1025, 0.6926, 0.8975, 0.8975], q:[0.2992], qb:[0.5041], phi:[0.2992]] [X:[[2]], M:[[3], [-9], [-3], [-3]], q:[[-1]], qb:[[5]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_2$, $ q_1\tilde{q}_1$, $ M_3$, $ M_4$, $ M_2^2$, $ X_1$, $ M_2q_1\tilde{q}_1$, $ M_2M_3$, $ M_2M_4$, $ q_1^2\tilde{q}_1^2$, $ M_3q_1\tilde{q}_1$, $ M_4q_1\tilde{q}_1$, $ M_3^2$, $ M_3M_4$, $ M_4^2$ . -2 t^2.08+t^2.41+2*t^2.69+t^4.16+t^4.2+t^4.49+2*t^4.77+t^4.82+2*t^5.1+2*t^5.39-2*t^6.+t^6.23+t^6.57-t^6.61+2*t^6.85+t^6.9+2*t^7.18+t^7.23+2*t^7.46+2*t^7.8-t^8.13+t^8.31-2*t^8.41+t^8.64-4*t^8.69+2*t^8.93-2*t^8.98-t^8.98/y^2-t^3.9/y-t^5.98/y-t^6.59/y+t^7.2/y+t^7.49/y+(2*t^7.77)/y+t^7.82/y-t^8.05/y+(2*t^8.1)/y+t^8.39/y-t^8.67/y-t^3.9*y-t^5.98*y-t^6.59*y+t^7.2*y+t^7.49*y+2*t^7.77*y+t^7.82*y-t^8.05*y+2*t^8.1*y+t^8.39*y-t^8.67*y-t^8.98*y^2 t^2.08/g1^9+g1^4*t^2.41+(2*t^2.69)/g1^3+t^4.16/g1^18+g1^2*t^4.2+t^4.49/g1^5+(2*t^4.77)/g1^12+g1^8*t^4.82+2*g1*t^5.1+(2*t^5.39)/g1^6-2*t^6.+t^6.23/g1^27+t^6.57/g1^14-g1^6*t^6.61+(2*t^6.85)/g1^21+t^6.9/g1+(2*t^7.18)/g1^8+g1^12*t^7.23+(2*t^7.46)/g1^15+(2*t^7.8)/g1^2-g1^11*t^8.13+t^8.31/g1^36-2*g1^4*t^8.41+t^8.64/g1^23-(4*t^8.69)/g1^3+(2*t^8.93)/g1^30-(2*t^8.98)/g1^10-t^8.98/(g1^10*y^2)-t^3.9/(g1*y)-t^5.98/(g1^10*y)-t^6.59/(g1^4*y)+(g1^2*t^7.2)/y+t^7.49/(g1^5*y)+(2*t^7.77)/(g1^12*y)+(g1^8*t^7.82)/y-t^8.05/(g1^19*y)+(2*g1*t^8.1)/y+t^8.39/(g1^6*y)-t^8.67/(g1^13*y)-(t^3.9*y)/g1-(t^5.98*y)/g1^10-(t^6.59*y)/g1^4+g1^2*t^7.2*y+(t^7.49*y)/g1^5+(2*t^7.77*y)/g1^12+g1^8*t^7.82*y-(t^8.05*y)/g1^19+2*g1*t^8.1*y+(t^8.39*y)/g1^6-(t^8.67*y)/g1^13-(t^8.98*y^2)/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
434 SU2adj1nf2 $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ + $ \phi_1^2X_1$ + $ M_3q_1q_2$ + $ M_1M_3$ + $ M_1M_4$ 0.4419 0.5359 0.8246 [X:[1.4016], M:[1.1025, 0.6926, 0.8975, 0.8975], q:[0.8504, 0.252], qb:[0.6455, 1.0553], phi:[0.2992]] t^2.08+t^2.41+2*t^2.69+t^4.16+t^4.2+t^4.49+2*t^4.77+t^4.82+2*t^5.1+2*t^5.39-2*t^6.-t^3.9/y-t^5.98/y-t^3.9*y-t^5.98*y detail


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
24 SU2adj1nf1 $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_3\phi_1q_1\tilde{q}_1$ + $ M_1M_3$ 0.4329 0.5202 0.8323 [X:[1.3957], M:[1.0936, 0.7193, 0.9064], q:[0.3021], qb:[0.4893], phi:[0.3021]] t^2.16+t^2.37+t^2.72+t^3.28+t^4.19+t^4.32+t^4.53+t^4.75+t^4.88+t^5.09+t^5.44+t^5.65-t^6.-t^3.91/y-t^3.91*y detail