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
46619 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ 0.7296 0.8971 0.8133 [M:[0.8907, 0.9842, 1.0158, 0.8907, 0.7657], q:[0.6639, 0.4454], qb:[0.5704, 0.5389], phi:[0.4454]] [M:[[-2, -2], [-1, 1], [1, -1], [-2, -2], [-5, -3]], q:[[3, 3], [-1, -1]], qb:[[2, 0], [0, 2]], phi:[[-1, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }M_{1}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$ ${}$ -3 t^2.297 + 3*t^2.672 + t^2.953 + t^3.047 + t^3.608 + t^4.008 + t^4.289 + t^4.383 + t^4.569 + t^4.594 + 2*t^4.664 + t^4.759 + t^4.944 + 3*t^4.969 + t^5.039 + t^5.25 + t^5.32 + 6*t^5.344 + t^5.625 + t^5.72 + t^5.905 - 3*t^6. + t^6.28 + t^6.305 - 2*t^6.375 + t^6.561 + t^6.586 - t^6.656 + 3*t^6.68 + t^6.866 + t^6.891 + 4*t^6.961 + 3*t^7.056 + t^7.217 + 4*t^7.241 + 3*t^7.266 + 4*t^7.336 + 3*t^7.431 + t^7.522 + t^7.547 + 3*t^7.617 + 6*t^7.641 + t^7.711 + t^7.806 + t^7.922 + 10*t^8.017 - t^8.086 + t^8.178 + t^8.202 - 2*t^8.297 - t^8.367 + t^8.392 + t^8.553 + t^8.578 + t^8.602 - t^8.647 - 10*t^8.672 + 2*t^8.858 + t^8.883 + t^8.928 - 2*t^8.953 + 3*t^8.978 - t^4.336/y - t^6.633/y - (3*t^7.008)/y + (3*t^7.664)/y + (3*t^7.969)/y + t^8.039/y + t^8.25/y + (4*t^8.344)/y + (3*t^8.625)/y + (3*t^8.72)/y + t^8.905/y - t^8.93/y - t^4.336*y - t^6.633*y - 3*t^7.008*y + 3*t^7.664*y + 3*t^7.969*y + t^8.039*y + t^8.25*y + 4*t^8.344*y + 3*t^8.625*y + 3*t^8.72*y + t^8.905*y - t^8.93*y t^2.297/(g1^5*g2^3) + (3*t^2.672)/(g1^2*g2^2) + (g2*t^2.953)/g1 + (g1*t^3.047)/g2 + g1^3*g2^5*t^3.608 + t^4.008/(g1^3*g2^3) + t^4.289/g1^2 + t^4.383/g2^2 + (g2^3*t^4.569)/g1 + t^4.594/(g1^10*g2^6) + 2*g1*g2*t^4.664 + (g1^3*t^4.759)/g2 + g1^2*g2^4*t^4.944 + (3*t^4.969)/(g1^7*g2^5) + g1^4*g2^2*t^5.039 + t^5.25/(g1^6*g2^2) + g1^5*g2^5*t^5.32 + (6*t^5.344)/(g1^4*g2^4) + t^5.625/(g1^3*g2) + t^5.72/(g1*g2^3) + (g2^2*t^5.905)/g1^2 - 3*t^6. + g1*g2^3*t^6.28 + t^6.305/(g1^8*g2^6) - 2*g1^3*g2*t^6.375 + g1^2*g2^6*t^6.561 + t^6.586/(g1^7*g2^3) - g1^4*g2^4*t^6.656 + (3*t^6.68)/(g1^5*g2^5) + t^6.866/g1^6 + t^6.891/(g1^15*g2^9) + (4*t^6.961)/(g1^4*g2^2) + (3*t^7.056)/(g1^2*g2^4) + g1^6*g2^10*t^7.217 + (4*g2*t^7.241)/g1^3 + (3*t^7.266)/(g1^12*g2^8) + (4*t^7.336)/(g1*g2) + (3*g1*t^7.431)/g2^3 + (g2^4*t^7.522)/g1^2 + t^7.547/(g1^11*g2^5) + 3*g2^2*t^7.617 + (6*t^7.641)/(g1^9*g2^7) + g1^2*t^7.711 + (g1^4*t^7.806)/g2^2 + t^7.922/(g1^8*g2^4) + (10*t^8.017)/(g1^6*g2^6) - g1^5*g2*t^8.086 + g1^2*g2^8*t^8.178 + t^8.202/(g1^7*g2) - (2*t^8.297)/(g1^5*g2^3) - g1^6*g2^4*t^8.367 + t^8.392/(g1^3*g2^5) + g1^5*g2^9*t^8.553 + t^8.578/g1^4 + t^8.602/(g1^13*g2^9) - g1^7*g2^7*t^8.647 - (10*t^8.672)/(g1^2*g2^2) + (2*g2^3*t^8.858)/g1^3 + t^8.883/(g1^12*g2^6) + g1^8*g2^10*t^8.928 - (2*g2*t^8.953)/g1 + (3*t^8.978)/(g1^10*g2^8) - t^4.336/(g1*g2*y) - t^6.633/(g1^6*g2^4*y) - (3*t^7.008)/(g1^3*g2^3*y) + (3*g1*g2*t^7.664)/y + (3*t^7.969)/(g1^7*g2^5*y) + (g1^4*g2^2*t^8.039)/y + t^8.25/(g1^6*g2^2*y) + (4*t^8.344)/(g1^4*g2^4*y) + (3*t^8.625)/(g1^3*g2*y) + (3*t^8.72)/(g1*g2^3*y) + (g2^2*t^8.905)/(g1^2*y) - t^8.93/(g1^11*g2^7*y) - (t^4.336*y)/(g1*g2) - (t^6.633*y)/(g1^6*g2^4) - (3*t^7.008*y)/(g1^3*g2^3) + 3*g1*g2*t^7.664*y + (3*t^7.969*y)/(g1^7*g2^5) + g1^4*g2^2*t^8.039*y + (t^8.25*y)/(g1^6*g2^2) + (4*t^8.344*y)/(g1^4*g2^4) + (3*t^8.625*y)/(g1^3*g2) + (3*t^8.72*y)/(g1*g2^3) + (g2^2*t^8.905*y)/g1^2 - (t^8.93*y)/(g1^11*g2^7)


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
47242 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ 0.6935 0.8487 0.8171 [M:[0.9891, 1.0327, 0.9673, 0.9891, 1.0109], q:[0.5163, 0.4946], qb:[0.4728, 0.5381], phi:[0.4946]] t^2.902 + 3*t^2.967 + t^3.033 + t^3.098 + t^3.163 + t^4.32 + t^4.386 + 2*t^4.451 + 2*t^4.516 + 2*t^4.582 + t^4.647 + t^4.712 + t^5.869 + 4*t^5.935 - t^4.484/y - t^4.484*y detail
47217 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ 0.7292 0.8958 0.814 [M:[0.8889, 1.0, 1.0, 0.8889, 0.7778], q:[0.6667, 0.4444], qb:[0.5556, 0.5556], phi:[0.4444]] t^2.333 + 3*t^2.667 + 2*t^3. + t^3.667 + t^4. + 2*t^4.333 + 5*t^4.667 + 5*t^5. + 8*t^5.333 + 2*t^5.667 - 2*t^6. - t^4.333/y - t^4.333*y detail {a: 35/48, c: 43/48, M1: 8/9, M2: 1, M3: 1, M4: 8/9, M5: 7/9, q1: 2/3, q2: 4/9, qb1: 5/9, qb2: 5/9, phi1: 4/9}
48153 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ 0.6976 0.853 0.8178 [M:[0.9741, 1.0517, 0.9483, 0.9741, 1.0], q:[0.5388, 0.4871], qb:[0.4612, 0.5647], phi:[0.4871]] t^2.845 + 3*t^2.922 + t^3. + t^3.155 + t^3.31 + t^4.228 + t^4.306 + t^4.384 + t^4.461 + 2*t^4.539 + t^4.616 + t^4.694 + t^4.772 + t^4.849 + t^5.767 + 6*t^5.845 + t^5.922 - 2*t^6. - t^4.461/y - t^4.461*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
46304 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ 0.7125 0.866 0.8228 [M:[0.9101, 1.0, 1.0, 0.9101], q:[0.6348, 0.4551], qb:[0.5449, 0.5449], phi:[0.4551]] 3*t^2.73 + 2*t^3. + 2*t^3.539 + t^4.095 + 2*t^4.365 + 4*t^4.635 + 2*t^4.905 + t^5.174 + 5*t^5.461 + 2*t^5.73 - 3*t^6. - t^4.365/y - t^4.365*y detail