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
58530 SU3adj1nf2 ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{3}$ 1.4456 1.6298 0.887 [X:[1.3521], M:[0.9131, 1.0281], q:[0.5086, 0.4499], qb:[0.5783, 0.5195], phi:[0.324]] [X:[[0, 4]], M:[[3, -7], [0, 6]], q:[[-2, 6], [1, 5]], qb:[[-1, 1], [2, 0]], phi:[[0, -2]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ ${}$ -3 t^2.74 + t^2.91 + 3*t^3.08 + t^3.88 + 3*t^4.06 + t^4.23 + t^4.85 + 2*t^5.03 + 2*t^5.2 + t^5.37 + t^5.48 + t^5.65 + 3*t^5.82 + 3*t^5.99 - 3*t^6. + 7*t^6.17 - 2*t^6.18 + t^6.34 + t^6.62 + t^6.79 + 2*t^6.8 + 7*t^6.96 - t^6.97 + 10*t^7.14 - 2*t^7.15 + 3*t^7.32 + t^7.49 + 2*t^7.59 + 2*t^7.76 + 6*t^7.94 + t^8.1 + 9*t^8.11 - t^8.12 + t^8.22 + 4*t^8.28 + 2*t^8.29 + t^8.39 + 3*t^8.46 + 2*t^8.56 + t^8.72 + 3*t^8.73 - 5*t^8.74 + 3*t^8.9 + 4*t^8.91 - 2*t^8.92 + t^8.92/y^2 - t^3.97/y - t^4.94/y - t^6.71/y - t^6.88/y - (3*t^7.06)/y - t^7.68/y - t^7.85/y - (3*t^8.03)/y + t^8.65/y + (2*t^8.82)/y + (3*t^8.99)/y - t^3.97*y - t^4.94*y - t^6.71*y - t^6.88*y - 3*t^7.06*y - t^7.68*y - t^7.85*y - 3*t^8.03*y + t^8.65*y + 2*t^8.82*y + 3*t^8.99*y + t^8.92*y^2 (g1^3*t^2.74)/g2^7 + g1^3*g2^5*t^2.91 + 3*g2^6*t^3.08 + g1^3*g2^3*t^3.88 + 3*g2^4*t^4.06 + (g2^5*t^4.23)/g1^3 + g1^3*g2*t^4.85 + 2*g2^2*t^5.03 + (g2^3*t^5.2)/g1^3 + g2^14*t^5.2 + (g2^15*t^5.37)/g1^3 + (g1^6*t^5.48)/g2^14 + (g1^6*t^5.65)/g2^2 + (2*g1^3*t^5.82)/g2 + g1^6*g2^10*t^5.82 + 3*g1^3*g2^11*t^5.99 - 3*t^6. + 7*g2^12*t^6.17 - (2*g2*t^6.18)/g1^3 + (g2^13*t^6.34)/g1^3 + (g1^6*t^6.62)/g2^4 + g1^6*g2^8*t^6.79 + (2*g1^3*t^6.8)/g2^3 + 7*g1^3*g2^9*t^6.96 - t^6.97/g2^2 + 10*g2^10*t^7.14 - (2*t^7.15)/(g1^3*g2) + (3*g2^11*t^7.32)/g1^3 + (g2^12*t^7.49)/g1^6 + (2*g1^6*t^7.59)/g2^6 + 2*g1^6*g2^6*t^7.76 - t^7.94/g2^4 + 7*g1^3*g2^7*t^7.94 + g1^3*g2^19*t^8.1 + 9*g2^8*t^8.11 - t^8.12/(g1^3*g2^3) + (g1^9*t^8.22)/g2^21 + 4*g2^20*t^8.28 + (2*g2^9*t^8.29)/g1^3 + (g1^9*t^8.39)/g2^9 + (3*g2^21*t^8.46)/g1^3 + (g1^6*t^8.56)/g2^8 + g1^9*g2^3*t^8.56 + g1^9*g2^15*t^8.72 + 3*g1^6*g2^4*t^8.73 - (5*g1^3*t^8.74)/g2^7 + 3*g1^6*g2^16*t^8.9 + 4*g1^3*g2^5*t^8.91 - (2*t^8.92)/g2^6 + t^8.92/(g2^6*y^2) - t^3.97/(g2^2*y) - t^4.94/(g2^4*y) - (g1^3*t^6.71)/(g2^9*y) - (g1^3*g2^3*t^6.88)/y - (3*g2^4*t^7.06)/y - (g1^3*t^7.68)/(g2^11*y) - (g1^3*g2*t^7.85)/y - (3*g2^2*t^8.03)/y + (g1^6*t^8.65)/(g2^2*y) + (2*g1^3*t^8.82)/(g2*y) + (3*g1^3*g2^11*t^8.99)/y - (t^3.97*y)/g2^2 - (t^4.94*y)/g2^4 - (g1^3*t^6.71*y)/g2^9 - g1^3*g2^3*t^6.88*y - 3*g2^4*t^7.06*y - (g1^3*t^7.68*y)/g2^11 - g1^3*g2*t^7.85*y - 3*g2^2*t^8.03*y + (g1^6*t^8.65*y)/g2^2 + (2*g1^3*t^8.82*y)/g2 + 3*g1^3*g2^11*t^8.99*y + (t^8.92*y^2)/g2^6


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
57394 SU3adj1nf2 ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ 1.4491 1.6312 0.8884 [X:[1.3648], M:[0.8988], q:[0.5224, 0.4683], qb:[0.5788, 0.5247], phi:[0.3176]] t^2.696 + t^2.859 + t^2.979 + 2*t^3.141 + t^3.932 + 3*t^4.094 + t^4.257 + t^4.885 + 2*t^5.047 + t^5.209 + t^5.33 + t^5.393 + t^5.492 + t^5.555 + t^5.675 + t^5.717 + 2*t^5.838 + t^5.958 - t^6. - t^3.953/y - t^4.906/y - t^3.953*y - t^4.906*y detail