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
46493 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ 0.5753 0.747 0.7701 [M:[0.6827, 0.76, 1.0387, 0.9613, 0.9613], q:[0.4938, 0.8235], qb:[0.7462, 0.2152], phi:[0.4303]] [M:[[1, 9], [-1, 7], [-1, -1], [1, 1], [1, 1]], q:[[0, -7], [-1, -2]], qb:[[1, 0], [0, 1]], phi:[[0, 2]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{2}^{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$ ${}\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}^{3}$ -2 t^2.048 + t^2.127 + t^2.28 + 2*t^2.582 + 2*t^2.884 + t^3.418 + t^4.096 + t^4.175 + 2*t^4.254 + t^4.328 + t^4.407 + t^4.56 + 2*t^4.63 + 3*t^4.709 + 2*t^4.862 + 2*t^4.932 + 2*t^5.011 + 4*t^5.164 + 4*t^5.466 + t^5.545 + 3*t^5.768 - 2*t^6. + t^6.144 + t^6.223 + 2*t^6.302 + t^6.376 + 2*t^6.381 + t^6.608 + 2*t^6.678 + t^6.687 + 2*t^6.757 + 2*t^6.836 + t^6.84 + 2*t^6.91 + 2*t^6.98 + 2*t^6.989 + 2*t^7.059 + 3*t^7.138 + 2*t^7.142 + 4*t^7.212 + 3*t^7.291 - t^7.37 + 4*t^7.444 + 4*t^7.514 + 4*t^7.593 + t^7.672 + 5*t^7.746 + 3*t^7.816 - 2*t^7.825 + 3*t^7.895 + 3*t^8.048 - 4*t^8.127 + t^8.193 + t^8.271 - 4*t^8.28 + 6*t^8.35 + t^8.424 + t^8.429 + 3*t^8.508 - 6*t^8.582 + 4*t^8.652 + t^8.656 - t^8.661 + 2*t^8.726 + 2*t^8.805 - 6*t^8.884 + t^8.888 + 2*t^8.958 + 2*t^8.963 + t^8.967 - t^4.291/y - t^6.339/y - t^6.571/y - t^6.873/y + t^7.328/y + (2*t^7.407)/y + (2*t^7.63)/y + (3*t^7.709)/y + (2*t^7.862)/y + (2*t^7.932)/y + (3*t^8.011)/y + (3*t^8.164)/y + t^8.243/y - t^8.387/y + (5*t^8.466)/y + t^8.545/y - t^8.619/y + t^8.698/y + t^8.768/y - t^8.851/y - t^8.921/y - t^4.291*y - t^6.339*y - t^6.571*y - t^6.873*y + t^7.328*y + 2*t^7.407*y + 2*t^7.63*y + 3*t^7.709*y + 2*t^7.862*y + 2*t^7.932*y + 3*t^8.011*y + 3*t^8.164*y + t^8.243*y - t^8.387*y + 5*t^8.466*y + t^8.545*y - t^8.619*y + t^8.698*y + t^8.768*y - t^8.851*y - t^8.921*y g1*g2^9*t^2.048 + t^2.127/g2^6 + (g2^7*t^2.28)/g1 + 2*g2^4*t^2.582 + 2*g1*g2*t^2.884 + t^3.418/g2^4 + g1^2*g2^18*t^4.096 + g1*g2^3*t^4.175 + (2*t^4.254)/g2^12 + g2^16*t^4.328 + (g2*t^4.407)/g1 + (g2^14*t^4.56)/g1^2 + 2*g1*g2^13*t^4.63 + (3*t^4.709)/g2^2 + (2*g2^11*t^4.862)/g1 + 2*g1^2*g2^10*t^4.932 + (2*g1*t^5.011)/g2^5 + 4*g2^8*t^5.164 + 4*g1*g2^5*t^5.466 + t^5.545/g2^10 + 3*g1^2*g2^2*t^5.768 - 2*t^6. + g1^3*g2^27*t^6.144 + g1^2*g2^12*t^6.223 + (2*g1*t^6.302)/g2^3 + g1*g2^25*t^6.376 + (2*t^6.381)/g2^18 + (g2^23*t^6.608)/g1 + 2*g1^2*g2^22*t^6.678 + (g2^8*t^6.687)/g1^2 + 2*g1*g2^7*t^6.757 + (2*t^6.836)/g2^8 + (g2^21*t^6.84)/g1^3 + 2*g2^20*t^6.91 + 2*g1^3*g2^19*t^6.98 + (2*g2^5*t^6.989)/g1 + 2*g1^2*g2^4*t^7.059 + (3*g1*t^7.138)/g2^11 + (2*g2^18*t^7.142)/g1^2 + 4*g1*g2^17*t^7.212 + 3*g2^2*t^7.291 - t^7.37/(g1*g2^13) + (4*g2^15*t^7.444)/g1 + 4*g1^2*g2^14*t^7.514 + (4*g1*t^7.593)/g2 + t^7.672/g2^16 + 5*g2^12*t^7.746 + 3*g1^3*g2^11*t^7.816 - (2*t^7.825)/(g1*g2^3) + (3*g1^2*t^7.895)/g2^4 + 3*g1*g2^9*t^8.048 - (4*t^8.127)/g2^6 + g1^4*g2^36*t^8.193 + g1^3*g2^21*t^8.271 - (4*g2^7*t^8.28)/g1 + 6*g1^2*g2^6*t^8.35 + g1^2*g2^34*t^8.424 + (g1*t^8.429)/g2^9 + (3*t^8.508)/g2^24 - 6*g2^4*t^8.582 + 4*g1^3*g2^3*t^8.652 + g2^32*t^8.656 - t^8.661/(g1*g2^11) + 2*g1^3*g2^31*t^8.726 + 2*g1^2*g2^16*t^8.805 - 6*g1*g2*t^8.884 + (g2^30*t^8.888)/g1^2 + 2*g1*g2^29*t^8.958 + (2*t^8.963)/g2^14 + (g2^15*t^8.967)/g1^3 - (g2^2*t^4.291)/y - (g1*g2^11*t^6.339)/y - (g2^9*t^6.571)/(g1*y) - (g2^6*t^6.873)/y + (g2^16*t^7.328)/y + (2*g2*t^7.407)/(g1*y) + (2*g1*g2^13*t^7.63)/y + (3*t^7.709)/(g2^2*y) + (2*g2^11*t^7.862)/(g1*y) + (2*g1^2*g2^10*t^7.932)/y + (3*g1*t^8.011)/(g2^5*y) + (3*g2^8*t^8.164)/y + t^8.243/(g1*g2^7*y) - (g1^2*g2^20*t^8.387)/y + (5*g1*g2^5*t^8.466)/y + t^8.545/(g2^10*y) - (g2^18*t^8.619)/y + (g2^3*t^8.698)/(g1*y) + (g1^2*g2^2*t^8.768)/y - (g2^16*t^8.851)/(g1^2*y) - (g1*g2^15*t^8.921)/y - g2^2*t^4.291*y - g1*g2^11*t^6.339*y - (g2^9*t^6.571*y)/g1 - g2^6*t^6.873*y + g2^16*t^7.328*y + (2*g2*t^7.407*y)/g1 + 2*g1*g2^13*t^7.63*y + (3*t^7.709*y)/g2^2 + (2*g2^11*t^7.862*y)/g1 + 2*g1^2*g2^10*t^7.932*y + (3*g1*t^8.011*y)/g2^5 + 3*g2^8*t^8.164*y + (t^8.243*y)/(g1*g2^7) - g1^2*g2^20*t^8.387*y + 5*g1*g2^5*t^8.466*y + (t^8.545*y)/g2^10 - g2^18*t^8.619*y + (g2^3*t^8.698*y)/g1 + g1^2*g2^2*t^8.768*y - (g2^16*t^8.851*y)/g1^2 - g1*g2^15*t^8.921*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


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
46205 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{5}$ 0.7284 0.8958 0.8131 [M:[0.7691, 0.8187, 1.0248, 0.9752, 0.9752], q:[0.6602, 0.5707], qb:[0.5212, 0.4541], phi:[0.4485]] t^2.307 + t^2.456 + t^2.691 + 2*t^2.926 + t^3.276 + t^3.343 + t^4.07 + t^4.271 + t^4.42 + t^4.472 + t^4.615 + t^4.621 + t^4.688 + t^4.763 + t^4.77 + t^4.889 + t^4.912 + t^4.998 + t^5.038 + t^5.147 + 2*t^5.233 + t^5.306 + 2*t^5.382 + 2*t^5.616 + 2*t^5.851 + t^5.967 - 4*t^6. - t^4.345/y - t^4.345*y detail