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
55703 SU2adj1nf3 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{3}\tilde{q}_{1}$ + ${ }M_{1}^{2}$ 0.856 1.0293 0.8316 [M:[1.0, 0.726], q:[0.75, 0.75, 0.637], qb:[0.637, 0.613, 0.613], phi:[0.5]] [M:[[0, 0, 0, 0], [0, 0, 1, 1]], q:[[-1, 0, 0, 0], [1, 0, 0, 0], [0, -1, -1, -1]], qb:[[0, 1, 0, 0], [0, 0, 1, 0], [0, 0, 0, 1]], phi:[[0, 0, 0, 0]]] 4
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }M_{1}$, ${ }\tilde{q}_{2}\tilde{q}_{3}$, ${ }q_{3}\tilde{q}_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{3}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{3}$, ${ }q_{2}\tilde{q}_{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{3}$, ${ }q_{2}q_{3}$, ${ }M_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{2}\tilde{q}_{3}$, ${ }\phi_{1}\tilde{q}_{3}^{2}$, ${ }\phi_{1}q_{3}\tilde{q}_{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{3}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{3}^{2}$, ${ }\phi_{1}q_{3}\tilde{q}_{1}$, ${ }M_{2}\tilde{q}_{2}\tilde{q}_{3}$ ${}$ -8 t^2.178 + t^3. + t^3.678 + 4*t^3.75 + 4*t^4.089 + 4*t^4.161 + t^4.356 + t^4.5 + 4*t^5.178 + 4*t^5.25 + 3*t^5.322 + t^5.856 - 8*t^6. - 4*t^6.072 + 4*t^6.267 - 4*t^6.411 + t^6.534 + 2*t^6.678 + 4*t^6.75 + 5*t^7.356 + 4*t^7.428 + 5*t^7.5 - 4*t^7.572 + 4*t^7.767 + 16*t^7.839 + 12*t^7.911 + t^8.034 + 5*t^8.178 + 16*t^8.25 + 12*t^8.322 + 4*t^8.445 - 4*t^8.589 + t^8.712 + 5*t^8.856 + 12*t^8.928 - t^4.5/y - t^6.678/y + t^8.178/y + t^8.322/y + (4*t^8.928)/y - t^4.5*y - t^6.678*y + t^8.178*y + t^8.322*y + 4*t^8.928*y g3*g4*t^2.178 + t^3. + g3*g4*t^3.678 + t^3.75/(g2*g3) + g2*g3*t^3.75 + t^3.75/(g2*g4) + g2*g4*t^3.75 + (g3*t^4.089)/g1 + g1*g3*t^4.089 + (g4*t^4.089)/g1 + g1*g4*t^4.089 + (g2*t^4.161)/g1 + g1*g2*t^4.161 + t^4.161/(g1*g2*g3*g4) + (g1*t^4.161)/(g2*g3*g4) + g3^2*g4^2*t^4.356 + t^4.5 + g3^2*t^5.178 + 2*g3*g4*t^5.178 + g4^2*t^5.178 + t^5.25/(g2*g3) + g2*g3*t^5.25 + t^5.25/(g2*g4) + g2*g4*t^5.25 + g2^2*t^5.322 + t^5.322/(g2^2*g3^2*g4^2) + t^5.322/(g3*g4) + g3^2*g4^2*t^5.856 - 4*t^6. - t^6./(g2^2*g3*g4) - (g3*t^6.)/g4 - (g4*t^6.)/g3 - g2^2*g3*g4*t^6. - (g2*t^6.072)/g3 - t^6.072/(g2*g3*g4^2) - (g2*t^6.072)/g4 - t^6.072/(g2*g3^2*g4) + (g3^2*g4*t^6.267)/g1 + g1*g3^2*g4*t^6.267 + (g3*g4^2*t^6.267)/g1 + g1*g3*g4^2*t^6.267 - t^6.411/(g1*g3) - (g1*t^6.411)/g3 - t^6.411/(g1*g4) - (g1*t^6.411)/g4 + g3^3*g4^3*t^6.534 + 2*g3*g4*t^6.678 + t^6.75/(g2*g3) + g2*g3*t^6.75 + t^6.75/(g2*g4) + g2*g4*t^6.75 + g3^3*g4*t^7.356 + 3*g3^2*g4^2*t^7.356 + g3*g4^3*t^7.356 + (g3*t^7.428)/g2 + (g4*t^7.428)/g2 + g2*g3^2*g4*t^7.428 + g2*g3*g4^2*t^7.428 - t^7.5 + t^7.5/(g2^2*g3^2) + g2^2*g3^2*t^7.5 + t^7.5/(g2^2*g4^2) + t^7.5/(g2^2*g3*g4) + g2^2*g3*g4*t^7.5 + g2^2*g4^2*t^7.5 - (g2*t^7.572)/g3 - t^7.572/(g2*g3*g4^2) - (g2*t^7.572)/g4 - t^7.572/(g2*g3^2*g4) + (g3^2*g4*t^7.767)/g1 + g1*g3^2*g4*t^7.767 + (g3*g4^2*t^7.767)/g1 + g1*g3*g4^2*t^7.767 + (2*t^7.839)/(g1*g2) + (2*g1*t^7.839)/g2 + (g2*g3^2*t^7.839)/g1 + g1*g2*g3^2*t^7.839 + (g3*t^7.839)/(g1*g2*g4) + (g1*g3*t^7.839)/(g2*g4) + (g4*t^7.839)/(g1*g2*g3) + (g1*g4*t^7.839)/(g2*g3) + (2*g2*g3*g4*t^7.839)/g1 + 2*g1*g2*g3*g4*t^7.839 + (g2*g4^2*t^7.839)/g1 + g1*g2*g4^2*t^7.839 + t^7.911/(g1*g3) + (g1*t^7.911)/g3 + (g2^2*g3*t^7.911)/g1 + g1*g2^2*g3*t^7.911 + t^7.911/(g1*g2^2*g3*g4^2) + (g1*t^7.911)/(g2^2*g3*g4^2) + t^7.911/(g1*g4) + (g1*t^7.911)/g4 + t^7.911/(g1*g2^2*g3^2*g4) + (g1*t^7.911)/(g2^2*g3^2*g4) + (g2^2*g4*t^7.911)/g1 + g1*g2^2*g4*t^7.911 + g3^3*g4^3*t^8.034 + (g3^2*t^8.178)/g1^2 + g1^2*g3^2*t^8.178 - g3*g4*t^8.178 + (g3*g4*t^8.178)/g1^2 + g1^2*g3*g4*t^8.178 + (g4^2*t^8.178)/g1^2 + g1^2*g4^2*t^8.178 + (2*t^8.25)/(g2*g3) + t^8.25/(g1^2*g2*g3) + (g1^2*t^8.25)/(g2*g3) + 2*g2*g3*t^8.25 + (g2*g3*t^8.25)/g1^2 + g1^2*g2*g3*t^8.25 + (2*t^8.25)/(g2*g4) + t^8.25/(g1^2*g2*g4) + (g1^2*t^8.25)/(g2*g4) + 2*g2*g4*t^8.25 + (g2*g4*t^8.25)/g1^2 + g1^2*g2*g4*t^8.25 + g2^2*t^8.322 + (g2^2*t^8.322)/g1^2 + g1^2*g2^2*t^8.322 + t^8.322/g3^2 + t^8.322/g4^2 + t^8.322/(g2^2*g3^2*g4^2) + t^8.322/(g1^2*g2^2*g3^2*g4^2) + (g1^2*t^8.322)/(g2^2*g3^2*g4^2) + (2*t^8.322)/(g3*g4) + t^8.322/(g1^2*g3*g4) + (g1^2*t^8.322)/(g3*g4) + (g3^3*g4^2*t^8.445)/g1 + g1*g3^3*g4^2*t^8.445 + (g3^2*g4^3*t^8.445)/g1 + g1*g3^2*g4^3*t^8.445 - (g3*t^8.589)/g1 - g1*g3*t^8.589 - (g4*t^8.589)/g1 - g1*g4*t^8.589 + g3^4*g4^4*t^8.712 + g3^3*g4*t^8.856 + 3*g3^2*g4^2*t^8.856 + g3*g4^3*t^8.856 + (2*g3*t^8.928)/g2 + g2*g3^3*t^8.928 + (g3^2*t^8.928)/(g2*g4) + (2*g4*t^8.928)/g2 + 2*g2*g3^2*g4*t^8.928 + (g4^2*t^8.928)/(g2*g3) + 2*g2*g3*g4^2*t^8.928 + g2*g4^3*t^8.928 - t^4.5/y - (g3*g4*t^6.678)/y + (g3*g4*t^8.178)/y + t^8.322/(g3*g4*y) + (g3*t^8.928)/(g2*y) + (g4*t^8.928)/(g2*y) + (g2*g3^2*g4*t^8.928)/y + (g2*g3*g4^2*t^8.928)/y - t^4.5*y - g3*g4*t^6.678*y + g3*g4*t^8.178*y + (t^8.322*y)/(g3*g4) + (g3*t^8.928*y)/g2 + (g4*t^8.928*y)/g2 + g2*g3^2*g4*t^8.928*y + g2*g3*g4^2*t^8.928*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
55680 SU2adj1nf3 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{3}\tilde{q}_{1}$ 0.8691 1.0645 0.8165 [M:[0.8785, 0.7991], q:[0.7196, 0.7196, 0.6005], qb:[0.6005, 0.5584, 0.5584], phi:[0.5607]] t^2.397 + t^2.636 + t^3.351 + 4*t^3.477 + 4*t^3.834 + 4*t^3.96 + t^4.318 + t^4.794 + 4*t^5.033 + 4*t^5.159 + t^5.271 + 3*t^5.285 + t^5.748 + t^5.986 - 9*t^6. - t^4.682/y - t^4.682*y detail