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
55915 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }M_{5}^{2}$ 0.6092 0.7767 0.7842 [M:[1.2857, 0.8901, 0.7143, 0.8242, 1.0, 0.7472], q:[0.4121, 0.3022], qb:[0.6978, 0.8736], phi:[0.4286]] [M:[[0], [2], [0], [-2], [0], [2]], q:[[-1], [1]], qb:[[-1], [1]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{6}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{6}\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$ ${}\phi_{1}^{3}q_{1}q_{2}$ 0 t^2.143 + t^2.242 + t^2.473 + t^2.571 + t^2.67 + t^3. + t^3.099 + t^3.429 + t^3.857 + t^4.286 + t^4.384 + t^4.483 + t^4.616 + 3*t^4.714 + 2*t^4.813 + t^4.912 + t^4.945 + t^5.044 + 3*t^5.143 + 3*t^5.242 + 2*t^5.34 + t^5.473 + 2*t^5.571 + 2*t^5.67 + t^5.769 + 2*t^6.099 + t^6.198 + t^6.429 + 2*t^6.527 + t^6.626 + t^6.725 + t^6.857 + 3*t^6.956 + 2*t^7.055 + t^7.088 + t^7.153 + t^7.187 + 3*t^7.286 + 5*t^7.384 + t^7.418 + 4*t^7.483 + t^7.517 + 2*t^7.582 + 2*t^7.616 + 5*t^7.714 + 5*t^7.813 + 4*t^7.912 + t^7.945 + 2*t^8.011 + t^8.242 + 4*t^8.34 + 2*t^8.439 - 3*t^8.473 + 3*t^8.769 + 2*t^8.868 - 2*t^8.901 + t^8.966 - t^4.286/y - t^6.527/y - t^6.758/y - t^6.857/y - t^6.956/y + t^7.384/y + (2*t^7.616)/y + (3*t^7.714)/y + (3*t^7.813)/y + t^7.912/y + (2*t^8.044)/y + (2*t^8.143)/y + (3*t^8.242)/y + t^8.34/y + t^8.473/y + (3*t^8.571)/y + (3*t^8.67)/y + t^8.901/y - t^4.286*y - t^6.527*y - t^6.758*y - t^6.857*y - t^6.956*y + t^7.384*y + 2*t^7.616*y + 3*t^7.714*y + 3*t^7.813*y + t^7.912*y + 2*t^8.044*y + 2*t^8.143*y + 3*t^8.242*y + t^8.34*y + t^8.473*y + 3*t^8.571*y + 3*t^8.67*y + t^8.901*y t^2.143 + g1^2*t^2.242 + t^2.473/g1^2 + t^2.571 + g1^2*t^2.67 + t^3. + g1^2*t^3.099 + t^3.429 + t^3.857 + t^4.286 + g1^2*t^4.384 + g1^4*t^4.483 + t^4.616/g1^2 + 3*t^4.714 + 2*g1^2*t^4.813 + g1^4*t^4.912 + t^4.945/g1^4 + t^5.044/g1^2 + 3*t^5.143 + 3*g1^2*t^5.242 + 2*g1^4*t^5.34 + t^5.473/g1^2 + 2*t^5.571 + 2*g1^2*t^5.67 + g1^4*t^5.769 + 2*g1^2*t^6.099 + g1^4*t^6.198 + t^6.429 + 2*g1^2*t^6.527 + g1^4*t^6.626 + g1^6*t^6.725 + t^6.857 + 3*g1^2*t^6.956 + 2*g1^4*t^7.055 + t^7.088/g1^4 + g1^6*t^7.153 + t^7.187/g1^2 + 3*t^7.286 + 5*g1^2*t^7.384 + t^7.418/g1^6 + 4*g1^4*t^7.483 + t^7.517/g1^4 + 2*g1^6*t^7.582 + (2*t^7.616)/g1^2 + 5*t^7.714 + 5*g1^2*t^7.813 + 4*g1^4*t^7.912 + t^7.945/g1^4 + 2*g1^6*t^8.011 + g1^2*t^8.242 + 4*g1^4*t^8.34 + 2*g1^6*t^8.439 - (3*t^8.473)/g1^2 + 3*g1^4*t^8.769 + 2*g1^6*t^8.868 - (2*t^8.901)/g1^2 + g1^8*t^8.966 - t^4.286/y - (g1^2*t^6.527)/y - t^6.758/(g1^2*y) - t^6.857/y - (g1^2*t^6.956)/y + (g1^2*t^7.384)/y + (2*t^7.616)/(g1^2*y) + (3*t^7.714)/y + (3*g1^2*t^7.813)/y + (g1^4*t^7.912)/y + (2*t^8.044)/(g1^2*y) + (2*t^8.143)/y + (3*g1^2*t^8.242)/y + (g1^4*t^8.34)/y + t^8.473/(g1^2*y) + (3*t^8.571)/y + (3*g1^2*t^8.67)/y + t^8.901/(g1^2*y) - t^4.286*y - g1^2*t^6.527*y - (t^6.758*y)/g1^2 - t^6.857*y - g1^2*t^6.956*y + g1^2*t^7.384*y + (2*t^7.616*y)/g1^2 + 3*t^7.714*y + 3*g1^2*t^7.813*y + g1^4*t^7.912*y + (2*t^8.044*y)/g1^2 + 2*t^8.143*y + 3*g1^2*t^8.242*y + g1^4*t^8.34*y + (t^8.473*y)/g1^2 + 3*t^8.571*y + 3*g1^2*t^8.67*y + (t^8.901*y)/g1^2


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
57537 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }M_{5}^{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ 0.614 0.7837 0.7835 [M:[1.2857, 0.9286, 0.7143, 0.7857, 1.0, 0.7857, 0.9286], q:[0.3929, 0.3214], qb:[0.6786, 0.8929], phi:[0.4286]] t^2.143 + 2*t^2.357 + t^2.571 + 2*t^2.786 + t^3. + t^3.429 + t^3.857 + t^4.286 + 2*t^4.5 + 5*t^4.714 + 4*t^4.929 + 6*t^5.143 + 4*t^5.357 + 4*t^5.571 + 2*t^5.786 - t^4.286/y - t^4.286*y detail {a: 13479/21952, c: 17203/21952, M1: 9/7, M2: 13/14, M3: 5/7, M4: 11/14, M5: 1, M6: 11/14, M7: 13/14, q1: 11/28, q2: 9/28, qb1: 19/28, qb2: 25/28, phi1: 3/7}


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
48168 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ 0.6733 0.8548 0.7876 [M:[1.1492, 0.7116, 0.8508, 0.8206, 0.6814, 0.7963], q:[0.4103, 0.4405], qb:[0.8781, 0.7389], phi:[0.3831]] t^2.044 + t^2.135 + t^2.298 + t^2.389 + t^2.462 + t^2.552 + t^3.448 + t^3.702 + t^3.792 + t^4.088 + t^4.179 + t^4.27 + t^4.343 + 2*t^4.433 + t^4.506 + t^4.524 + 3*t^4.597 + 2*t^4.687 + t^4.76 + t^4.778 + 3*t^4.851 + t^4.924 + t^4.941 + t^5.014 + t^5.105 + t^5.492 + t^5.582 + t^5.746 + 2*t^5.836 + t^5.927 - t^6. - t^4.149/y - t^4.149*y detail