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
734 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}q_{2}$ 0.7163 0.8881 0.8066 [M:[1.0, 0.9211, 1.0, 0.7481, 0.6692], q:[0.7913, 0.5394], qb:[0.4606, 0.5394], phi:[0.4173]] [M:[[0], [-14], [0], [6], [-8]], q:[[1], [7]], qb:[[-7], [7]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}^{2}$ ${}M_{1}M_{3}$, ${ }M_{5}q_{1}\tilde{q}_{2}$ -1 t^2.008 + t^2.244 + t^2.504 + t^2.763 + 2*t^3. + t^3.992 + 2*t^4.015 + 3*t^4.252 + 4*t^4.489 + t^4.511 + t^4.748 + t^4.771 + 4*t^5.008 + 2*t^5.244 + t^5.267 + 2*t^5.504 + t^5.527 - t^6. + 2*t^6.023 - t^6.237 + 3*t^6.26 + 5*t^6.496 + 2*t^6.519 + 4*t^6.733 + 2*t^6.756 + 2*t^6.779 + 4*t^6.992 + 6*t^7.015 + 6*t^7.252 + t^7.275 + 4*t^7.489 + 3*t^7.511 + t^7.534 + 2*t^7.771 - 2*t^7.985 + 4*t^8.031 - 5*t^8.244 + 5*t^8.267 + t^8.29 + 5*t^8.504 + 2*t^8.527 + 5*t^8.74 - t^8.763 + 2*t^8.786 + 9*t^8.977 - t^4.252/y - t^6.26/y - t^6.496/y - t^6.756/y - t^7.015/y + t^7.252/y + t^7.489/y + t^7.511/y + (2*t^7.748)/y + t^7.771/y + (4*t^8.008)/y + (3*t^8.244)/y + t^8.504/y - t^8.74/y + t^8.763/y - t^4.252*y - t^6.26*y - t^6.496*y - t^6.756*y - t^7.015*y + t^7.252*y + t^7.489*y + t^7.511*y + 2*t^7.748*y + t^7.771*y + 4*t^8.008*y + 3*t^8.244*y + t^8.504*y - t^8.74*y + t^8.763*y t^2.008/g1^8 + g1^6*t^2.244 + t^2.504/g1^4 + t^2.763/g1^14 + 2*t^3. + g1^8*t^3.992 + (2*t^4.015)/g1^16 + (3*t^4.252)/g1^2 + 4*g1^12*t^4.489 + t^4.511/g1^12 + g1^2*t^4.748 + t^4.771/g1^22 + (4*t^5.008)/g1^8 + 2*g1^6*t^5.244 + t^5.267/g1^18 + (2*t^5.504)/g1^4 + t^5.527/g1^28 - t^6. + (2*t^6.023)/g1^24 - g1^14*t^6.237 + (3*t^6.26)/g1^10 + 5*g1^4*t^6.496 + (2*t^6.519)/g1^20 + 4*g1^18*t^6.733 + (2*t^6.756)/g1^6 + (2*t^6.779)/g1^30 + 4*g1^8*t^6.992 + (6*t^7.015)/g1^16 + (6*t^7.252)/g1^2 + t^7.275/g1^26 + 4*g1^12*t^7.489 + (3*t^7.511)/g1^12 + t^7.534/g1^36 + (2*t^7.771)/g1^22 - 2*g1^16*t^7.985 + (4*t^8.031)/g1^32 - 5*g1^6*t^8.244 + (5*t^8.267)/g1^18 + t^8.29/g1^42 + (5*t^8.504)/g1^4 + (2*t^8.527)/g1^28 + 5*g1^10*t^8.74 - t^8.763/g1^14 + (2*t^8.786)/g1^38 + 9*g1^24*t^8.977 - t^4.252/(g1^2*y) - t^6.26/(g1^10*y) - (g1^4*t^6.496)/y - t^6.756/(g1^6*y) - t^7.015/(g1^16*y) + t^7.252/(g1^2*y) + (g1^12*t^7.489)/y + t^7.511/(g1^12*y) + (2*g1^2*t^7.748)/y + t^7.771/(g1^22*y) + (4*t^8.008)/(g1^8*y) + (3*g1^6*t^8.244)/y + t^8.504/(g1^4*y) - (g1^10*t^8.74)/y + t^8.763/(g1^14*y) - (t^4.252*y)/g1^2 - (t^6.26*y)/g1^10 - g1^4*t^6.496*y - (t^6.756*y)/g1^6 - (t^7.015*y)/g1^16 + (t^7.252*y)/g1^2 + g1^12*t^7.489*y + (t^7.511*y)/g1^12 + 2*g1^2*t^7.748*y + (t^7.771*y)/g1^22 + (4*t^8.008*y)/g1^8 + 3*g1^6*t^8.244*y + (t^8.504*y)/g1^4 - g1^10*t^8.74*y + (t^8.763*y)/g1^14


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
1205 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ 0.7372 0.9296 0.793 [M:[1.0, 0.9207, 1.0, 0.7483, 0.669, 0.669], q:[0.7914, 0.5397], qb:[0.4603, 0.5397], phi:[0.4172]] 2*t^2.007 + t^2.245 + t^2.503 + t^2.762 + 2*t^3. + 4*t^4.014 + 4*t^4.252 + 4*t^4.49 + 2*t^4.51 + t^4.748 + 2*t^4.769 + 6*t^5.007 + 2*t^5.245 + t^5.265 + 2*t^5.503 + t^5.524 - 2*t^6. - t^4.252/y - t^4.252*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
439 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ 0.6955 0.8466 0.8215 [M:[1.0, 0.9217, 1.0, 0.7479], q:[0.7913, 0.5392], qb:[0.4608, 0.5392], phi:[0.4174]] t^2.244 + t^2.504 + t^2.765 + 2*t^3. + 2*t^3.991 + t^4.017 + 2*t^4.252 + 4*t^4.487 + t^4.748 + 2*t^5.009 + 2*t^5.244 + t^5.269 + 2*t^5.504 + t^5.53 - 2*t^6. - t^4.252/y - t^4.252*y detail