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
46907 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ 0.6259 0.8118 0.7711 [M:[1.0, 0.9469, 0.7301, 0.7301, 1.0531], q:[0.7566, 0.2434], qb:[0.5133, 0.5398], phi:[0.4867]] [M:[[0], [-8], [-3], [-3], [8]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}^{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$ -2 2*t^2.19 + t^2.27 + t^2.35 + 2*t^2.92 + t^3. + t^3.159 + t^3.73 + t^3.889 + 3*t^4.381 + 2*t^4.46 + 4*t^4.54 + 2*t^4.619 + 2*t^4.699 + 3*t^5.111 + 3*t^5.19 + 3*t^5.27 + 3*t^5.35 + t^5.429 + t^5.509 + 3*t^5.841 + 2*t^5.92 - 2*t^6. + 3*t^6.08 + t^6.159 + t^6.239 + t^6.319 + 3*t^6.571 + 3*t^6.65 + 5*t^6.73 + 4*t^6.81 + 6*t^6.889 + 2*t^6.969 + 3*t^7.049 + 4*t^7.301 + 3*t^7.381 + 6*t^7.46 + 5*t^7.54 + 5*t^7.619 + 4*t^7.699 + 2*t^7.779 + 2*t^7.858 + 4*t^8.031 + 3*t^8.111 - 2*t^8.19 + 2*t^8.27 - 3*t^8.35 + 3*t^8.429 + 3*t^8.509 + 3*t^8.588 + t^8.668 + 8*t^8.761 + 3*t^8.841 - t^4.46/y - (2*t^6.65)/y + (2*t^7.46)/y + (3*t^7.54)/y + t^7.619/y + (4*t^8.111)/y + (4*t^8.19)/y + (5*t^8.27)/y + (3*t^8.35)/y + t^8.429/y + t^8.509/y - (2*t^8.841)/y + (4*t^8.92)/y - t^4.46*y - 2*t^6.65*y + 2*t^7.46*y + 3*t^7.54*y + t^7.619*y + 4*t^8.111*y + 4*t^8.19*y + 5*t^8.27*y + 3*t^8.35*y + t^8.429*y + t^8.509*y - 2*t^8.841*y + 4*t^8.92*y (2*t^2.19)/g1^3 + g1*t^2.27 + g1^5*t^2.35 + (2*t^2.92)/g1^4 + t^3. + g1^8*t^3.159 + t^3.73/g1 + g1^7*t^3.889 + (3*t^4.381)/g1^6 + (2*t^4.46)/g1^2 + 4*g1^2*t^4.54 + 2*g1^6*t^4.619 + 2*g1^10*t^4.699 + (3*t^5.111)/g1^7 + (3*t^5.19)/g1^3 + 3*g1*t^5.27 + 3*g1^5*t^5.35 + g1^9*t^5.429 + g1^13*t^5.509 + (3*t^5.841)/g1^8 + (2*t^5.92)/g1^4 - 2*t^6. + 3*g1^4*t^6.08 + g1^8*t^6.159 + g1^12*t^6.239 + g1^16*t^6.319 + (3*t^6.571)/g1^9 + (3*t^6.65)/g1^5 + (5*t^6.73)/g1 + 4*g1^3*t^6.81 + 6*g1^7*t^6.889 + 2*g1^11*t^6.969 + 3*g1^15*t^7.049 + (4*t^7.301)/g1^10 + (3*t^7.381)/g1^6 + (6*t^7.46)/g1^2 + 5*g1^2*t^7.54 + 5*g1^6*t^7.619 + 4*g1^10*t^7.699 + 2*g1^14*t^7.779 + 2*g1^18*t^7.858 + (4*t^8.031)/g1^11 + (3*t^8.111)/g1^7 - (2*t^8.19)/g1^3 + 2*g1*t^8.27 - 3*g1^5*t^8.35 + 3*g1^9*t^8.429 + 3*g1^13*t^8.509 + 3*g1^17*t^8.588 + g1^21*t^8.668 + (8*t^8.761)/g1^12 + (3*t^8.841)/g1^8 - t^4.46/(g1^2*y) - (2*t^6.65)/(g1^5*y) + (2*t^7.46)/(g1^2*y) + (3*g1^2*t^7.54)/y + (g1^6*t^7.619)/y + (4*t^8.111)/(g1^7*y) + (4*t^8.19)/(g1^3*y) + (5*g1*t^8.27)/y + (3*g1^5*t^8.35)/y + (g1^9*t^8.429)/y + (g1^13*t^8.509)/y - (2*t^8.841)/(g1^8*y) + (4*t^8.92)/(g1^4*y) - (t^4.46*y)/g1^2 - (2*t^6.65*y)/g1^5 + (2*t^7.46*y)/g1^2 + 3*g1^2*t^7.54*y + g1^6*t^7.619*y + (4*t^8.111*y)/g1^7 + (4*t^8.19*y)/g1^3 + 5*g1*t^8.27*y + 3*g1^5*t^8.35*y + g1^9*t^8.429*y + g1^13*t^8.509*y - (2*t^8.841*y)/g1^8 + (4*t^8.92*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
55357 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{6}\phi_{1}^{2}$ 0.6242 0.8106 0.7701 [M:[1.0, 0.9818, 0.7432, 0.7432, 1.0182, 1.0091], q:[0.7523, 0.2477], qb:[0.5045, 0.5136], phi:[0.4955]] 2*t^2.23 + t^2.257 + t^2.284 + t^2.973 + t^3. + t^3.027 + t^3.054 + t^3.743 + t^3.798 + 3*t^4.459 + 2*t^4.486 + 4*t^4.514 + 2*t^4.541 + 2*t^4.568 + t^5.202 + 2*t^5.23 + 4*t^5.257 + 4*t^5.284 + 2*t^5.311 + t^5.339 + t^5.946 + t^5.973 - t^6. - t^4.486/y - t^4.486*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
46670 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ 0.6338 0.825 0.7683 [M:[1.0, 0.8827, 0.706, 0.706], q:[0.7647, 0.2353], qb:[0.5293, 0.5879], phi:[0.4707]] 2*t^2.118 + t^2.294 + t^2.47 + t^2.648 + 2*t^2.824 + t^3. + t^3.706 + t^4.058 + 3*t^4.236 + 2*t^4.412 + 4*t^4.588 + 2*t^4.764 + 2*t^4.766 + 2*t^4.94 + 4*t^4.942 + 4*t^5.118 + 3*t^5.294 + t^5.296 + t^5.47 + 2*t^5.472 + 4*t^5.648 + 2*t^5.824 - 2*t^6. - t^4.412/y - t^4.412*y detail