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
689 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ 0.688 0.8539 0.8058 [M:[1.0, 1.1155, 0.9801, 0.769, 0.6931], q:[0.7789, 0.4323], qb:[0.5677, 0.4522], phi:[0.4422]] [M:[[0], [4], [-18], [-8], [24]], q:[[1], [-11]], qb:[[11], [7]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{4}q_{1}q_{2}$ ${}$ -1 t^2.079 + t^2.307 + t^2.653 + t^2.94 + t^3. + t^3.347 + t^3.634 + t^3.98 + 2*t^4.04 + t^4.159 + t^4.327 + 2*t^4.386 + t^4.614 + 2*t^4.733 + t^4.96 + t^5.02 + t^5.079 + t^5.247 + 2*t^5.307 + t^5.426 + t^5.653 + t^5.713 + t^5.881 + t^5.94 - t^6. + 2*t^6.119 + t^6.238 + 2*t^6.287 + t^6.347 + 2*t^6.466 + t^6.574 + 2*t^6.634 + 3*t^6.693 + 2*t^6.812 + t^6.921 + 2*t^6.98 + 3*t^7.04 + t^7.099 + t^7.159 + t^7.267 + t^7.327 + 3*t^7.386 + t^7.505 + t^7.554 + 2*t^7.614 + t^7.673 + t^7.733 + t^7.792 + 3*t^7.96 + 2*t^8.02 + t^8.079 + t^8.188 + 2*t^8.199 + t^8.247 - 2*t^8.307 + t^8.318 + 2*t^8.366 + 2*t^8.426 + 2*t^8.545 + t^8.594 + 5*t^8.773 + t^8.821 + t^8.881 + 2*t^8.892 - t^4.327/y - t^6.406/y - t^6.634/y - t^7.267/y + (2*t^7.386)/y + t^7.733/y + t^7.96/y + (2*t^8.02)/y + t^8.079/y + (2*t^8.247)/y + t^8.307/y + t^8.426/y - t^8.486/y + t^8.594/y + (2*t^8.653)/y + t^8.94/y - t^4.327*y - t^6.406*y - t^6.634*y - t^7.267*y + 2*t^7.386*y + t^7.733*y + t^7.96*y + 2*t^8.02*y + t^8.079*y + 2*t^8.247*y + t^8.307*y + t^8.426*y - t^8.486*y + t^8.594*y + 2*t^8.653*y + t^8.94*y g1^24*t^2.079 + t^2.307/g1^8 + t^2.653/g1^4 + t^2.94/g1^18 + t^3. + g1^4*t^3.347 + t^3.634/g1^10 + t^3.98/g1^6 + 2*g1^12*t^4.04 + g1^48*t^4.159 + t^4.327/g1^2 + 2*g1^16*t^4.386 + t^4.614/g1^16 + 2*g1^20*t^4.733 + t^4.96/g1^12 + g1^6*t^5.02 + g1^24*t^5.079 + t^5.247/g1^26 + (2*t^5.307)/g1^8 + g1^28*t^5.426 + t^5.653/g1^4 + g1^14*t^5.713 + t^5.881/g1^36 + t^5.94/g1^18 - t^6. + 2*g1^36*t^6.119 + g1^72*t^6.238 + (2*t^6.287)/g1^14 + g1^4*t^6.347 + 2*g1^40*t^6.466 + t^6.574/g1^28 + (2*t^6.634)/g1^10 + 3*g1^8*t^6.693 + 2*g1^44*t^6.812 + t^6.921/g1^24 + (2*t^6.98)/g1^6 + 3*g1^12*t^7.04 + g1^30*t^7.099 + g1^48*t^7.159 + t^7.267/g1^20 + t^7.327/g1^2 + 3*g1^16*t^7.386 + g1^52*t^7.505 + t^7.554/g1^34 + (2*t^7.614)/g1^16 + g1^2*t^7.673 + g1^20*t^7.733 + g1^38*t^7.792 + (3*t^7.96)/g1^12 + 2*g1^6*t^8.02 + g1^24*t^8.079 + t^8.188/g1^44 + 2*g1^60*t^8.199 + t^8.247/g1^26 - (2*t^8.307)/g1^8 + g1^96*t^8.318 + 2*g1^10*t^8.366 + 2*g1^28*t^8.426 + 2*g1^64*t^8.545 + t^8.594/g1^22 + 5*g1^32*t^8.773 + t^8.821/g1^54 + t^8.881/g1^36 + 2*g1^68*t^8.892 - t^4.327/(g1^2*y) - (g1^22*t^6.406)/y - t^6.634/(g1^10*y) - t^7.267/(g1^20*y) + (2*g1^16*t^7.386)/y + (g1^20*t^7.733)/y + t^7.96/(g1^12*y) + (2*g1^6*t^8.02)/y + (g1^24*t^8.079)/y + (2*t^8.247)/(g1^26*y) + t^8.307/(g1^8*y) + (g1^28*t^8.426)/y - (g1^46*t^8.486)/y + t^8.594/(g1^22*y) + (2*t^8.653)/(g1^4*y) + t^8.94/(g1^18*y) - (t^4.327*y)/g1^2 - g1^22*t^6.406*y - (t^6.634*y)/g1^10 - (t^7.267*y)/g1^20 + 2*g1^16*t^7.386*y + g1^20*t^7.733*y + (t^7.96*y)/g1^12 + 2*g1^6*t^8.02*y + g1^24*t^8.079*y + (2*t^8.247*y)/g1^26 + (t^8.307*y)/g1^8 + g1^28*t^8.426*y - g1^46*t^8.486*y + (t^8.594*y)/g1^22 + (2*t^8.653*y)/g1^4 + (t^8.94*y)/g1^18


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
417 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ 0.6675 0.8146 0.8194 [M:[1.0, 1.118, 0.9688, 0.7639], q:[0.7795, 0.4254], qb:[0.5746, 0.4566], phi:[0.441]] t^2.292 + t^2.646 + t^2.907 + t^3. + t^3.354 + t^3.615 + t^3.875 + t^3.969 + 2*t^4.062 + t^4.323 + t^4.416 + t^4.584 + t^4.771 + t^4.938 + t^5.198 + 2*t^5.292 + t^5.646 + t^5.813 + t^5.907 - t^6. - t^4.323/y - t^4.323*y detail