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
661 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}q_{1}q_{2}$ 0.6695 0.8304 0.8062 [M:[0.8506, 1.1494, 0.977, 0.7241, 0.8506], q:[0.7874, 0.4885], qb:[0.6609, 0.3621], phi:[0.4253]] [M:[[-4], [4], [-14], [6], [-4]], q:[[1], [-7]], qb:[[11], [3]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$ ${}M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ 3 t^2.172 + 3*t^2.552 + t^2.931 + 2*t^3.448 + t^3.828 + t^4.207 + 3*t^4.345 + 4*t^4.724 + 6*t^5.104 + t^5.241 + 2*t^5.483 + t^5.621 + t^5.862 + 3*t^6. + 2*t^6.379 + 2*t^6.517 + 3*t^6.759 + 6*t^6.896 + t^7.138 + 7*t^7.276 + t^7.414 + 9*t^7.655 + 4*t^7.793 + 5*t^8.035 - t^8.172 + 3*t^8.414 + 4*t^8.689 + t^8.793 + t^8.931 - t^4.276/y - t^6.448/y - (2*t^6.828)/y - t^7.207/y + t^7.345/y + (5*t^7.724)/y + (5*t^8.104)/y + (3*t^8.483)/y + t^8.621/y - t^4.276*y - t^6.448*y - 2*t^6.828*y - t^7.207*y + t^7.345*y + 5*t^7.724*y + 5*t^8.104*y + 3*t^8.483*y + t^8.621*y g1^6*t^2.172 + (3*t^2.552)/g1^4 + t^2.931/g1^14 + 2*g1^4*t^3.448 + t^3.828/g1^6 + t^4.207/g1^16 + 3*g1^12*t^4.345 + 4*g1^2*t^4.724 + (6*t^5.104)/g1^8 + g1^20*t^5.241 + (2*t^5.483)/g1^18 + g1^10*t^5.621 + t^5.862/g1^28 + 3*t^6. + (2*t^6.379)/g1^10 + 2*g1^18*t^6.517 + (3*t^6.759)/g1^20 + 6*g1^8*t^6.896 + t^7.138/g1^30 + (7*t^7.276)/g1^2 + g1^26*t^7.414 + (9*t^7.655)/g1^12 + 4*g1^16*t^7.793 + (5*t^8.035)/g1^22 - g1^6*t^8.172 + (3*t^8.414)/g1^32 + 4*g1^24*t^8.689 + t^8.793/g1^42 + t^8.931/g1^14 - t^4.276/(g1^2*y) - (g1^4*t^6.448)/y - (2*t^6.828)/(g1^6*y) - t^7.207/(g1^16*y) + (g1^12*t^7.345)/y + (5*g1^2*t^7.724)/y + (5*t^8.104)/(g1^8*y) + (3*t^8.483)/(g1^18*y) + (g1^10*t^8.621)/y - (t^4.276*y)/g1^2 - g1^4*t^6.448*y - (2*t^6.828*y)/g1^6 - (t^7.207*y)/g1^16 + g1^12*t^7.345*y + 5*g1^2*t^7.724*y + (5*t^8.104*y)/g1^8 + (3*t^8.483*y)/g1^18 + g1^10*t^8.621*y


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
1054 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}q_{1}q_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ 0.6465 0.809 0.7991 [M:[0.8, 1.2, 0.8, 0.8, 0.8], q:[0.8, 0.4], qb:[0.8, 0.4], phi:[0.4]] 5*t^2.4 + 4*t^3.6 + 16*t^4.8 + 11*t^6. - t^4.2/y - t^4.2*y detail {a: 1293/2000, c: 809/1000, M1: 4/5, M2: 6/5, M3: 4/5, M4: 4/5, M5: 4/5, q1: 4/5, q2: 2/5, qb1: 4/5, qb2: 2/5, phi1: 2/5}
1053 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}q_{1}q_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ 0.6827 0.8534 0.8 [M:[0.8464, 1.1536, 0.9625, 0.7304, 0.8464, 0.8464], q:[0.7884, 0.4812], qb:[0.6723, 0.3652], phi:[0.4232]] t^2.191 + 4*t^2.539 + t^2.887 + t^3.461 + t^3.809 + t^4.157 + 3*t^4.382 + 5*t^4.73 + 10*t^5.079 + t^5.304 + 3*t^5.427 + t^5.775 + t^6. - t^4.27/y - t^4.27*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
411 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ 0.6814 0.8416 0.8096 [M:[0.9657, 1.1263, 0.9657, 0.6895, 0.8737], q:[0.7816, 0.4368], qb:[0.5974, 0.4368], phi:[0.4368]] t^2.069 + 2*t^2.621 + 2*t^2.897 + 2*t^3.655 + 2*t^3.931 + 2*t^4.137 + 2*t^4.413 + 2*t^4.69 + t^4.895 + 2*t^4.966 + 3*t^5.242 + 2*t^5.518 + 2*t^5.724 + 3*t^5.794 - 3*t^6. - t^4.31/y - t^4.31*y detail