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
58719 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ 1.1471 1.3549 0.8466 [X:[1.3511], M:[0.7022], q:[0.9867, 0.3378], qb:[0.3378, 0.3111], phi:[0.3378]] [X:[[4]], M:[[8]], q:[[-3], [1]], qb:[[1], [-5]], phi:[[1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{5}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${2}\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ 2}\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ 2}\phi_{1}^{3}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ 6 2*t^2.03 + t^2.11 + t^2.96 + 2*t^3.04 + t^3.89 + 3*t^3.97 + 4*t^4.05 + 2*t^4.13 + t^4.21 + 2*t^4.91 + 3*t^4.99 + 4*t^5.07 + 2*t^5.15 + t^5.84 + 3*t^5.92 + 6*t^6. + 11*t^6.08 + 4*t^6.16 + 2*t^6.24 + t^6.32 + t^6.85 + 4*t^6.93 + 10*t^7.01 + 8*t^7.09 + 4*t^7.17 + 2*t^7.25 + t^7.79 + 4*t^7.87 + 10*t^7.95 + 11*t^8.03 + 16*t^8.11 + 11*t^8.19 + 4*t^8.27 + 2*t^8.35 + t^8.43 + 2*t^8.8 + 6*t^8.88 + 4*t^8.96 - t^4.01/y - t^5.03/y - (2*t^6.04)/y - t^6.12/y - (2*t^7.05)/y + t^7.13/y + t^7.99/y - t^8.23/y + (2*t^8.92)/y - t^4.01*y - t^5.03*y - 2*t^6.04*y - t^6.12*y - 2*t^7.05*y + t^7.13*y + t^7.99*y - t^8.23*y + 2*t^8.92*y 2*g1^2*t^2.03 + g1^8*t^2.11 + t^2.96/g1^3 + 2*g1^3*t^3.04 + t^3.89/g1^8 + (3*t^3.97)/g1^2 + 4*g1^4*t^4.05 + 2*g1^10*t^4.13 + g1^16*t^4.21 + (2*t^4.91)/g1^7 + (3*t^4.99)/g1 + 4*g1^5*t^5.07 + 2*g1^11*t^5.15 + t^5.84/g1^12 + (3*t^5.92)/g1^6 + 6*t^6. + 11*g1^6*t^6.08 + 4*g1^12*t^6.16 + 2*g1^18*t^6.24 + g1^24*t^6.32 + t^6.85/g1^11 + (4*t^6.93)/g1^5 + 10*g1*t^7.01 + 8*g1^7*t^7.09 + 4*g1^13*t^7.17 + 2*g1^19*t^7.25 + t^7.79/g1^16 + (4*t^7.87)/g1^10 + (10*t^7.95)/g1^4 + 11*g1^2*t^8.03 + 16*g1^8*t^8.11 + 11*g1^14*t^8.19 + 4*g1^20*t^8.27 + 2*g1^26*t^8.35 + g1^32*t^8.43 + (2*t^8.8)/g1^15 + (6*t^8.88)/g1^9 + (4*t^8.96)/g1^3 - (g1*t^4.01)/y - (g1^2*t^5.03)/y - (2*g1^3*t^6.04)/y - (g1^9*t^6.12)/y - (2*g1^4*t^7.05)/y + (g1^10*t^7.13)/y + t^7.99/(g1*y) - (g1^17*t^8.23)/y + (2*t^8.92)/(g1^6*y) - g1*t^4.01*y - g1^2*t^5.03*y - 2*g1^3*t^6.04*y - g1^9*t^6.12*y - 2*g1^4*t^7.05*y + g1^10*t^7.13*y + (t^7.99*y)/g1 - g1^17*t^8.23*y + (2*t^8.92*y)/g1^6


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
57581 SU3adj1nf2 ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ 1.1267 1.3165 0.8559 [X:[1.3575], M:[], q:[0.9819, 0.3394], qb:[0.3394, 0.3031], phi:[0.3394]] 2*t^2.04 + t^2.95 + 2*t^3.05 + 2*t^3.85 + 3*t^3.96 + 4*t^4.07 + 2*t^4.87 + 3*t^4.98 + 3*t^5.09 + t^5.78 + 5*t^5.89 + 5*t^6. - t^4.02/y - t^5.04/y - t^4.02*y - t^5.04*y detail