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
50937 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ 0.5959 0.7583 0.7859 [M:[0.9025, 1.0975, 1.0, 0.9025, 0.7075, 0.805], q:[0.6037, 0.4938], qb:[0.2988, 0.9938], phi:[0.4025]] [M:[[-2], [2], [0], [-2], [-6], [-4]], q:[[-3], [5]], qb:[[1], [5]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{4}$ ${}$ -2 t^2.122 + t^2.378 + 2*t^2.415 + 2*t^2.707 + t^3. + t^4.17 + t^4.245 + t^4.463 + t^4.5 + 2*t^4.537 + t^4.755 + 3*t^4.793 + 5*t^4.83 + 2*t^5.085 + 4*t^5.122 + t^5.378 + 4*t^5.415 + t^5.707 - 2*t^6. - t^6.293 - t^6.33 + t^6.367 + t^6.548 + t^6.585 + 2*t^6.66 + t^6.84 + 3*t^6.878 + 2*t^6.915 + 5*t^6.952 + t^7.133 + 3*t^7.17 + 5*t^7.207 + 8*t^7.245 + 2*t^7.463 + 4*t^7.5 + 8*t^7.537 + 3*t^7.793 + 6*t^7.83 - t^8.048 - t^8.085 + t^8.122 + t^8.34 - 4*t^8.378 - 4*t^8.415 - t^8.452 + t^8.49 + t^8.633 - 2*t^8.67 - 7*t^8.707 - t^8.745 + 2*t^8.782 + 2*t^8.925 + t^8.963 - t^4.207/y - t^6.33/y - (2*t^6.622)/y - t^6.915/y + (2*t^7.5)/y + (2*t^7.537)/y + (4*t^7.793)/y + (3*t^7.83)/y + (3*t^8.085)/y + (5*t^8.122)/y + t^8.378/y + (3*t^8.415)/y - t^8.452/y + (2*t^8.707)/y - (2*t^8.745)/y - t^4.207*y - t^6.33*y - 2*t^6.622*y - t^6.915*y + 2*t^7.5*y + 2*t^7.537*y + 4*t^7.793*y + 3*t^7.83*y + 3*t^8.085*y + 5*t^8.122*y + t^8.378*y + 3*t^8.415*y - t^8.452*y + 2*t^8.707*y - 2*t^8.745*y t^2.122/g1^6 + g1^6*t^2.378 + (2*t^2.415)/g1^4 + (2*t^2.707)/g1^2 + t^3. + g1^8*t^4.17 + t^4.245/g1^12 + g1^10*t^4.463 + t^4.5 + (2*t^4.537)/g1^10 + g1^12*t^4.755 + 3*g1^2*t^4.793 + (5*t^4.83)/g1^8 + 2*g1^4*t^5.085 + (4*t^5.122)/g1^6 + g1^6*t^5.378 + (4*t^5.415)/g1^4 + t^5.707/g1^2 - 2*t^6. - g1^2*t^6.293 - t^6.33/g1^8 + t^6.367/g1^18 + g1^14*t^6.548 + g1^4*t^6.585 + (2*t^6.66)/g1^16 + g1^16*t^6.84 + 3*g1^6*t^6.878 + (2*t^6.915)/g1^4 + (5*t^6.952)/g1^14 + g1^18*t^7.133 + 3*g1^8*t^7.17 + (5*t^7.207)/g1^2 + (8*t^7.245)/g1^12 + 2*g1^10*t^7.463 + 4*t^7.5 + (8*t^7.537)/g1^10 + 3*g1^2*t^7.793 + (6*t^7.83)/g1^8 - g1^14*t^8.048 - g1^4*t^8.085 + t^8.122/g1^6 + g1^16*t^8.34 - 4*g1^6*t^8.378 - (4*t^8.415)/g1^4 - t^8.452/g1^14 + t^8.49/g1^24 + g1^18*t^8.633 - 2*g1^8*t^8.67 - (7*t^8.707)/g1^2 - t^8.745/g1^12 + (2*t^8.782)/g1^22 + 2*g1^20*t^8.925 + g1^10*t^8.963 - t^4.207/(g1^2*y) - t^6.33/(g1^8*y) - (2*t^6.622)/(g1^6*y) - t^6.915/(g1^4*y) + (2*t^7.5)/y + (2*t^7.537)/(g1^10*y) + (4*g1^2*t^7.793)/y + (3*t^7.83)/(g1^8*y) + (3*g1^4*t^8.085)/y + (5*t^8.122)/(g1^6*y) + (g1^6*t^8.378)/y + (3*t^8.415)/(g1^4*y) - t^8.452/(g1^14*y) + (2*t^8.707)/(g1^2*y) - (2*t^8.745)/(g1^12*y) - (t^4.207*y)/g1^2 - (t^6.33*y)/g1^8 - (2*t^6.622*y)/g1^6 - (t^6.915*y)/g1^4 + 2*t^7.5*y + (2*t^7.537*y)/g1^10 + 4*g1^2*t^7.793*y + (3*t^7.83*y)/g1^8 + 3*g1^4*t^8.085*y + (5*t^8.122*y)/g1^6 + g1^6*t^8.378*y + (3*t^8.415*y)/g1^4 - (t^8.452*y)/g1^14 + (2*t^8.707*y)/g1^2 - (2*t^8.745*y)/g1^12


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
47223 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ 0.5801 0.7306 0.794 [M:[0.9081, 1.0919, 1.0, 0.9081, 0.7242], q:[0.6121, 0.4799], qb:[0.296, 0.9799], phi:[0.4081]] t^2.173 + t^2.327 + t^2.448 + 2*t^2.724 + t^3. + t^3.552 + t^4.103 + t^4.345 + t^4.379 + t^4.5 + t^4.621 + t^4.655 + 2*t^4.776 + 3*t^4.897 + 2*t^5.052 + 2*t^5.173 + t^5.327 + 3*t^5.448 + 2*t^5.724 + t^5.879 - t^6. - t^4.224/y - t^4.224*y detail