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
55531 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{6}$ 0.6243 0.8105 0.7702 [M:[1.0, 0.9796, 0.7372, 1.0102, 0.7474, 1.0204], q:[0.7526, 0.2474], qb:[0.5102, 0.5102], phi:[0.4949]] [M:[[0], [-8], [-5], [4], [-1], [8]], q:[[1], [-1]], qb:[[4], [4]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{4}$, ${ }M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ ${}M_{4}\phi_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ -2 t^2.212 + t^2.242 + 2*t^2.273 + t^2.969 + t^3. + t^3.031 + t^3.061 + t^3.758 + t^3.788 + t^4.423 + t^4.454 + 3*t^4.485 + 2*t^4.515 + 6*t^4.546 + t^5.181 + 4*t^5.242 + 4*t^5.273 + 3*t^5.304 + 2*t^5.334 + t^5.939 + t^5.969 - 2*t^6. + 4*t^6.031 + 3*t^6.061 + t^6.092 + t^6.122 + t^6.635 + t^6.666 + t^6.696 + 2*t^6.727 + 6*t^6.758 + 4*t^6.788 + 10*t^6.819 + t^6.849 + t^7.393 + 3*t^7.454 - t^7.485 + 8*t^7.515 + 8*t^7.546 + 6*t^7.577 + 6*t^7.607 + t^8.151 - 2*t^8.212 - t^8.242 - 5*t^8.273 + 8*t^8.304 + 8*t^8.334 + 3*t^8.365 + 2*t^8.395 + t^8.847 + t^8.878 + 2*t^8.908 + 3*t^8.939 - t^8.969 - t^4.485/y - t^6.696/y - t^6.727/y + t^7.454/y + (2*t^7.485)/y + (2*t^7.515)/y + t^7.546/y + t^8.181/y + (2*t^8.212)/y + (5*t^8.242)/y + (5*t^8.273)/y + (3*t^8.304)/y + (2*t^8.334)/y - t^8.908/y - t^8.939/y + t^8.969/y - t^4.485*y - t^6.696*y - t^6.727*y + t^7.454*y + 2*t^7.485*y + 2*t^7.515*y + t^7.546*y + t^8.181*y + 2*t^8.212*y + 5*t^8.242*y + 5*t^8.273*y + 3*t^8.304*y + 2*t^8.334*y - t^8.908*y - t^8.939*y + t^8.969*y t^2.212/g1^5 + t^2.242/g1 + 2*g1^3*t^2.273 + t^2.969/g1^4 + t^3. + g1^4*t^3.031 + g1^8*t^3.061 + g1*t^3.758 + g1^5*t^3.788 + t^4.423/g1^10 + t^4.454/g1^6 + (3*t^4.485)/g1^2 + 2*g1^2*t^4.515 + 6*g1^6*t^4.546 + t^5.181/g1^9 + (4*t^5.242)/g1 + 4*g1^3*t^5.273 + 3*g1^7*t^5.304 + 2*g1^11*t^5.334 + t^5.939/g1^8 + t^5.969/g1^4 - 2*t^6. + 4*g1^4*t^6.031 + 3*g1^8*t^6.061 + g1^12*t^6.092 + g1^16*t^6.122 + t^6.635/g1^15 + t^6.666/g1^11 + t^6.696/g1^7 + (2*t^6.727)/g1^3 + 6*g1*t^6.758 + 4*g1^5*t^6.788 + 10*g1^9*t^6.819 + g1^13*t^6.849 + t^7.393/g1^14 + (3*t^7.454)/g1^6 - t^7.485/g1^2 + 8*g1^2*t^7.515 + 8*g1^6*t^7.546 + 6*g1^10*t^7.577 + 6*g1^14*t^7.607 + t^8.151/g1^13 - (2*t^8.212)/g1^5 - t^8.242/g1 - 5*g1^3*t^8.273 + 8*g1^7*t^8.304 + 8*g1^11*t^8.334 + 3*g1^15*t^8.365 + 2*g1^19*t^8.395 + t^8.847/g1^20 + t^8.878/g1^16 + (2*t^8.908)/g1^12 + (3*t^8.939)/g1^8 - t^8.969/g1^4 - t^4.485/(g1^2*y) - t^6.696/(g1^7*y) - t^6.727/(g1^3*y) + t^7.454/(g1^6*y) + (2*t^7.485)/(g1^2*y) + (2*g1^2*t^7.515)/y + (g1^6*t^7.546)/y + t^8.181/(g1^9*y) + (2*t^8.212)/(g1^5*y) + (5*t^8.242)/(g1*y) + (5*g1^3*t^8.273)/y + (3*g1^7*t^8.304)/y + (2*g1^11*t^8.334)/y - t^8.908/(g1^12*y) - t^8.939/(g1^8*y) + t^8.969/(g1^4*y) - (t^4.485*y)/g1^2 - (t^6.696*y)/g1^7 - (t^6.727*y)/g1^3 + (t^7.454*y)/g1^6 + (2*t^7.485*y)/g1^2 + 2*g1^2*t^7.515*y + g1^6*t^7.546*y + (t^8.181*y)/g1^9 + (2*t^8.212*y)/g1^5 + (5*t^8.242*y)/g1 + 5*g1^3*t^8.273*y + 3*g1^7*t^8.304*y + 2*g1^11*t^8.334*y - (t^8.908*y)/g1^12 - (t^8.939*y)/g1^8 + (t^8.969*y)/g1^4


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
57112 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{4}M_{7}$ 0.6261 0.8118 0.7713 [M:[1.0, 0.941, 0.7131, 1.0295, 0.7426, 1.059, 0.9705], q:[0.7574, 0.2426], qb:[0.5295, 0.5295], phi:[0.4852]] t^2.139 + t^2.228 + 2*t^2.316 + 2*t^2.911 + t^3. + t^3.177 + t^3.772 + t^3.861 + t^4.279 + t^4.367 + 3*t^4.456 + 2*t^4.544 + 6*t^4.633 + 2*t^5.051 + t^5.139 + 5*t^5.228 + 3*t^5.316 + t^5.405 + 2*t^5.494 + 3*t^5.823 + 2*t^5.911 - 3*t^6. - t^4.456/y - t^4.456*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
47144 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ 0.6296 0.8171 0.7705 [M:[1.0, 0.9072, 0.692, 1.0464, 0.7384], q:[0.7616, 0.2384], qb:[0.5464, 0.5464], phi:[0.4768]] t^2.076 + t^2.215 + 2*t^2.354 + t^2.722 + t^2.861 + t^3. + t^3.139 + t^3.785 + t^3.924 + t^4.152 + t^4.291 + 3*t^4.43 + 2*t^4.57 + 6*t^4.709 + t^4.798 + 2*t^4.937 + 2*t^5.076 + 4*t^5.215 + 3*t^5.354 + t^5.443 + 2*t^5.494 + t^5.582 + 2*t^5.722 + 2*t^5.861 - 2*t^6. - t^4.43/y - t^4.43*y detail