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
3391 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{5}M_{6}$ 0.6685 0.8456 0.7906 [M:[0.7228, 0.8331, 0.7228, 0.8331, 1.1669, 0.8331], q:[0.8607, 0.4165], qb:[0.4165, 0.7504], phi:[0.389]] [M:[[14], [-6], [14], [-6], [6], [-6]], q:[[-11], [-3]], qb:[[-3], [9]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ ${}\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$ -2 2*t^2.168 + t^2.334 + 3*t^2.499 + 3*t^3.666 + 3*t^4.337 + 2*t^4.502 + 7*t^4.668 + 4*t^4.833 + 6*t^4.999 + 4*t^5.835 - 2*t^6. + 7*t^6.165 + 4*t^6.505 + 3*t^6.671 + 11*t^6.836 + 7*t^7.001 + 10*t^7.167 + 8*t^7.332 + 8*t^7.498 + 5*t^8.003 - 6*t^8.168 + 5*t^8.334 - 9*t^8.499 + 10*t^8.665 + 5*t^8.674 + 4*t^8.839 - t^4.167/y - (2*t^6.335)/y - t^6.501/y - (2*t^6.666)/y + t^7.337/y + (2*t^7.502)/y + (8*t^7.668)/y + (4*t^7.833)/y + (5*t^7.999)/y - (3*t^8.504)/y - (2*t^8.669)/y + t^8.835/y - t^4.167*y - 2*t^6.335*y - t^6.501*y - 2*t^6.666*y + t^7.337*y + 2*t^7.502*y + 8*t^7.668*y + 4*t^7.833*y + 5*t^7.999*y - 3*t^8.504*y - 2*t^8.669*y + t^8.835*y 2*g1^14*t^2.168 + g1^4*t^2.334 + (3*t^2.499)/g1^6 + (3*t^3.666)/g1^4 + 3*g1^28*t^4.337 + 2*g1^18*t^4.502 + 7*g1^8*t^4.668 + (4*t^4.833)/g1^2 + (6*t^4.999)/g1^12 + 4*g1^10*t^5.835 - 2*t^6. + (7*t^6.165)/g1^10 + 4*g1^42*t^6.505 + 3*g1^32*t^6.671 + 11*g1^22*t^6.836 + 7*g1^12*t^7.001 + 10*g1^2*t^7.167 + (8*t^7.332)/g1^8 + (8*t^7.498)/g1^18 + 5*g1^24*t^8.003 - 6*g1^14*t^8.168 + 5*g1^4*t^8.334 - (9*t^8.499)/g1^6 + (10*t^8.665)/g1^16 + 5*g1^56*t^8.674 + 4*g1^46*t^8.839 - (g1^2*t^4.167)/y - (2*g1^16*t^6.335)/y - (g1^6*t^6.501)/y - (2*t^6.666)/(g1^4*y) + (g1^28*t^7.337)/y + (2*g1^18*t^7.502)/y + (8*g1^8*t^7.668)/y + (4*t^7.833)/(g1^2*y) + (5*t^7.999)/(g1^12*y) - (3*g1^30*t^8.504)/y - (2*g1^20*t^8.669)/y + (g1^10*t^8.835)/y - g1^2*t^4.167*y - 2*g1^16*t^6.335*y - g1^6*t^6.501*y - (2*t^6.666*y)/g1^4 + g1^28*t^7.337*y + 2*g1^18*t^7.502*y + 8*g1^8*t^7.668*y + (4*t^7.833*y)/g1^2 + (5*t^7.999*y)/g1^12 - 3*g1^30*t^8.504*y - 2*g1^20*t^8.669*y + g1^10*t^8.835*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
3871 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ 0.6509 0.814 0.7996 [M:[0.7307, 0.8297, 0.7307, 0.8297, 1.1703, 0.8297, 1.2198], q:[0.8544, 0.4148], qb:[0.4148, 0.7555], phi:[0.3901]] 2*t^2.192 + 3*t^2.489 + 4*t^3.659 + 3*t^4.384 + 6*t^4.681 + t^4.83 + 6*t^4.978 + 6*t^5.852 - 5*t^6. - t^4.17/y - t^4.17*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
2840 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ 0.6544 0.8219 0.7962 [M:[0.7069, 0.8399, 0.7069, 0.8399, 1.1601], q:[0.8732, 0.42], qb:[0.42, 0.7401], phi:[0.3867]] 2*t^2.121 + t^2.32 + 2*t^2.52 + t^3.48 + 3*t^3.68 + 3*t^4.241 + 2*t^4.441 + 5*t^4.64 + 3*t^4.84 + 3*t^5.039 + 2*t^5.601 + 5*t^5.8 - t^4.16/y - t^4.16*y detail