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
521 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{1}^{2}$ 0.6965 0.8595 0.8103 [M:[1.0, 1.0541, 0.9459, 0.9459, 0.9459], q:[0.4459, 0.5541], qb:[0.5, 0.5], phi:[0.5]] [M:[[0, 0], [1, 1], [-1, -1], [-1, 1], [-1, -1]], q:[[-1, 0], [1, 0]], qb:[[0, -1], [0, 1]], phi:[[0, 0]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{5}$, ${ }M_{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ ${}M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ -1 4*t^2.838 + 3*t^3. + t^4.175 + 2*t^4.338 + 4*t^4.5 + 2*t^4.662 + t^4.825 + 9*t^5.675 + 8*t^5.838 - t^6. - 4*t^6.162 - t^6.325 + 4*t^7.013 + 8*t^7.175 + 12*t^7.338 + 6*t^7.5 + t^8.351 + 18*t^8.513 + 17*t^8.675 - 6*t^8.838 - t^4.5/y - (2*t^7.338)/y + (2*t^7.662)/y + (6*t^8.675)/y + (12*t^8.838)/y - t^4.5*y - 2*t^7.338*y + 2*t^7.662*y + 6*t^8.675*y + 12*t^8.838*y (2*t^2.838)/(g1*g2) + (2*g2*t^2.838)/g1 + 3*t^3. + t^4.175/g1^2 + t^4.338/(g1*g2) + (g2*t^4.338)/g1 + 2*t^4.5 + t^4.5/g2^2 + g2^2*t^4.5 + (g1*t^4.662)/g2 + g1*g2*t^4.662 + g1^2*t^4.825 + (3*t^5.675)/g1^2 + (3*t^5.675)/(g1^2*g2^2) + (3*g2^2*t^5.675)/g1^2 + (4*t^5.838)/(g1*g2) + (4*g2*t^5.838)/g1 + t^6. - t^6./g2^2 - g2^2*t^6. - (2*g1*t^6.162)/g2 - 2*g1*g2*t^6.162 - g1^2*t^6.325 + (2*t^7.013)/(g1^3*g2) + (2*g2*t^7.013)/g1^3 + (4*t^7.175)/g1^2 + (2*t^7.175)/(g1^2*g2^2) + (2*g2^2*t^7.175)/g1^2 + (2*t^7.338)/(g1*g2^3) + (4*t^7.338)/(g1*g2) + (4*g2*t^7.338)/g1 + (2*g2^3*t^7.338)/g1 + 2*t^7.5 + (2*t^7.5)/g2^2 + 2*g2^2*t^7.5 + t^8.351/g1^4 + (4*t^8.513)/(g1^3*g2^3) + (5*t^8.513)/(g1^3*g2) + (5*g2*t^8.513)/g1^3 + (4*g2^3*t^8.513)/g1^3 + (5*t^8.675)/g1^2 + (6*t^8.675)/(g1^2*g2^2) + (6*g2^2*t^8.675)/g1^2 - t^8.838/(g1*g2^3) - (2*t^8.838)/(g1*g2) - (2*g2*t^8.838)/g1 - (g2^3*t^8.838)/g1 - t^4.5/y - t^7.338/(g1*g2*y) - (g2*t^7.338)/(g1*y) + (g1*t^7.662)/(g2*y) + (g1*g2*t^7.662)/y + (4*t^8.675)/(g1^2*y) + t^8.675/(g1^2*g2^2*y) + (g2^2*t^8.675)/(g1^2*y) + (6*t^8.838)/(g1*g2*y) + (6*g2*t^8.838)/(g1*y) - t^4.5*y - (t^7.338*y)/(g1*g2) - (g2*t^7.338*y)/g1 + (g1*t^7.662*y)/g2 + g1*g2*t^7.662*y + (4*t^8.675*y)/g1^2 + (t^8.675*y)/(g1^2*g2^2) + (g2^2*t^8.675*y)/g1^2 + (6*t^8.838*y)/(g1*g2) + (6*g2*t^8.838*y)/g1


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
332 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ 0.7566 0.9235 0.8193 [M:[0.7979, 0.8325, 0.7634, 0.7634, 1.1675], q:[0.5665, 0.6356], qb:[0.601, 0.601], phi:[0.399]] 2*t^2.29 + 2*t^2.394 + 2*t^3.503 + t^3.606 + 3*t^4.58 + t^4.596 + 4*t^4.684 + 2*t^4.699 + 3*t^4.788 + 4*t^4.803 + 2*t^4.907 + t^5.01 + 3*t^5.793 + 2*t^5.896 - 4*t^6. - t^4.197/y - t^4.197*y detail