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
58430 SU3adj1nf2 ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ 1.4148 1.606 0.8809 [X:[1.4114], M:[0.7057, 0.7659], q:[0.5769, 0.5167], qb:[0.7174, 0.4231], phi:[0.2943]] [X:[[0, 2]], M:[[0, 1], [0, -6]], q:[[-1, 0], [-1, 7]], qb:[[1, -1], [1, 0]], phi:[[0, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }M_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }X_{1}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$ ${}$ -2 t^2.12 + t^2.3 + t^2.65 + t^2.82 + t^3. + t^3.7 + t^3.88 + 2*t^4.23 + t^4.41 + 2*t^4.59 + t^4.6 + 3*t^4.77 + t^4.94 + t^4.95 + t^5.12 + 2*t^5.3 + 2*t^5.47 + t^5.57 + t^5.64 + 2*t^5.65 + t^5.71 + t^5.82 + t^5.89 - 2*t^6. + 3*t^6.35 + 3*t^6.46 + t^6.52 + 3*t^6.53 + t^6.6 + 3*t^6.7 + t^6.71 + t^6.78 + 2*t^6.88 + t^6.89 + 2*t^7.05 + 2*t^7.06 - t^7.13 + 4*t^7.23 + t^7.24 + t^7.3 + 2*t^7.34 + 3*t^7.4 + 4*t^7.41 + t^7.48 + 6*t^7.59 + 2*t^7.6 + t^7.66 - t^7.69 + t^7.76 + 3*t^7.77 + t^7.84 - t^7.87 + t^7.94 + 2*t^7.95 - t^8.01 + 2*t^8.22 + 4*t^8.29 + t^8.36 + t^8.39 + t^8.46 + 9*t^8.47 + t^8.53 + t^8.54 + t^8.57 + t^8.64 + 3*t^8.65 + t^8.71 - 2*t^8.82 + 2*t^8.83 - t^8.89 + t^8.65/y^2 - t^3.88/y - t^4.77/y - t^6./y - t^6.18/y - t^6.53/y - t^6.7/y - (2*t^6.88)/y - t^7.06/y - t^7.59/y + t^7.94/y + t^7.95/y + t^8.12/y - t^8.48/y - t^8.65/y + t^8.82/y - t^8.83/y - t^3.88*y - t^4.77*y - t^6.*y - t^6.18*y - t^6.53*y - t^6.7*y - 2*t^6.88*y - t^7.06*y - t^7.59*y + t^7.94*y + t^7.95*y + t^8.12*y - t^8.48*y - t^8.65*y + t^8.82*y - t^8.83*y + t^8.65*y^2 g2*t^2.12 + t^2.3/g2^6 + t^2.65/g2^3 + g2^7*t^2.82 + t^3. + g2^6*t^3.7 + t^3.88/g2 + 2*g2^2*t^4.23 + t^4.41/g2^5 + 2*g2^5*t^4.59 + t^4.6/g2^12 + (3*t^4.77)/g2^2 + g2^8*t^4.94 + t^4.95/g2^9 + g2*t^5.12 + (2*t^5.3)/g2^6 + 2*g2^4*t^5.47 + (g1^3*t^5.57)/g2^2 + g2^14*t^5.64 + (2*t^5.65)/g2^3 + (g2^13*t^5.71)/g1^3 + g2^7*t^5.82 + (g2^6*t^5.89)/g1^3 - 2*t^6. + 3*g2^3*t^6.35 + (3*g1^3*t^6.46)/g2^3 + g2^13*t^6.52 + (3*t^6.53)/g2^4 + (g2^12*t^6.6)/g1^3 + 3*g2^6*t^6.7 + t^6.71/g2^11 + (g2^5*t^6.78)/g1^3 + (2*t^6.88)/g2 + t^6.89/g2^18 + 2*g2^9*t^7.05 + (2*t^7.06)/g2^8 - (g2^8*t^7.13)/g1^3 + 4*g2^2*t^7.23 + t^7.24/g2^15 + (g2^18*t^7.3)/g1^3 + (2*g1^3*t^7.34)/g2^4 + 3*g2^12*t^7.4 + (4*t^7.41)/g2^5 + (g2^11*t^7.48)/g1^3 + 6*g2^5*t^7.59 + (2*t^7.6)/g2^12 + (g2^4*t^7.66)/g1^3 - (g1^3*t^7.69)/g2 + g2^15*t^7.76 + (3*t^7.77)/g2^2 + t^7.84/(g1^3*g2^3) - (g1^3*t^7.87)/g2^8 + g2^8*t^7.94 + (2*t^7.95)/g2^9 - (g2^7*t^8.01)/g1^3 + (2*g1^3*t^8.22)/g2^5 + 4*g2^11*t^8.29 + (g2^10*t^8.36)/g1^3 + g1^3*g2^5*t^8.39 + g2^21*t^8.46 + 9*g2^4*t^8.47 + (g2^20*t^8.53)/g1^3 + (g2^3*t^8.54)/g1^3 + (g1^3*t^8.57)/g2^2 + g2^14*t^8.64 + (3*t^8.65)/g2^3 + (g2^13*t^8.71)/g1^3 - 2*g2^7*t^8.82 + (2*t^8.83)/g2^10 - (g2^6*t^8.89)/g1^3 + t^8.65/(g2^3*y^2) - t^3.88/(g2*y) - t^4.77/(g2^2*y) - t^6./y - t^6.18/(g2^7*y) - t^6.53/(g2^4*y) - (g2^6*t^6.7)/y - (2*t^6.88)/(g2*y) - t^7.06/(g2^8*y) - (g2^5*t^7.59)/y + (g2^8*t^7.94)/y + t^7.95/(g2^9*y) + (g2*t^8.12)/y - t^8.48/(g2^13*y) - t^8.65/(g2^3*y) + (g2^7*t^8.82)/y - t^8.83/(g2^10*y) - (t^3.88*y)/g2 - (t^4.77*y)/g2^2 - t^6.*y - (t^6.18*y)/g2^7 - (t^6.53*y)/g2^4 - g2^6*t^6.7*y - (2*t^6.88*y)/g2 - (t^7.06*y)/g2^8 - g2^5*t^7.59*y + g2^8*t^7.94*y + (t^7.95*y)/g2^9 + g2*t^8.12*y - (t^8.48*y)/g2^13 - (t^8.65*y)/g2^3 + g2^7*t^8.82*y - (t^8.83*y)/g2^10 + (t^8.65*y^2)/g2^3


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
57371 SU3adj1nf2 ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ 1.422 1.6203 0.8776 [X:[1.3791], M:[0.7761, 0.7761], q:[0.5214, 0.5214], qb:[0.7025, 0.392], phi:[0.3104]] 2*t^2.328 + 2*t^2.74 + t^2.794 + 2*t^3.672 + t^4.137 + 4*t^4.603 + 3*t^4.657 + 3*t^5.069 + 2*t^5.122 + t^5.391 + 3*t^5.481 + 4*t^5.534 + t^5.588 + 2*t^5.624 - 3*t^6. - t^3.931/y - t^4.863/y - t^3.931*y - t^4.863*y detail