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
2264 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{1}M_{7}$ 0.6469 0.8121 0.7965 [M:[1.2069, 0.8161, 0.7931, 0.7931, 0.7816, 1.1839, 0.7931], q:[0.7988, 0.385], qb:[0.4081, 0.7988], phi:[0.4023]] [M:[[-6], [-14], [6], [6], [16], [14], [6]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{5}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{6}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{7}q_{1}q_{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{7}\phi_{1}q_{2}\tilde{q}_{1}$ ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ -2 t^2.345 + 3*t^2.379 + t^2.414 + t^3.517 + 2*t^3.552 + t^3.586 + t^4.69 + 3*t^4.724 + 7*t^4.759 + 4*t^4.793 + t^4.828 + t^5.862 + 5*t^5.896 + 7*t^5.931 + 3*t^5.965 - 2*t^6. - 2*t^6.035 - t^6.069 + 2*t^7.034 + 5*t^7.069 + 10*t^7.103 + 13*t^7.138 + 6*t^7.172 - 2*t^7.241 - t^7.276 + t^8.207 + 5*t^8.241 + 13*t^8.276 + 15*t^8.31 + 4*t^8.345 - 9*t^8.379 - 10*t^8.414 - 6*t^8.448 - t^8.483 - t^4.207/y - t^6.552/y - (2*t^6.586)/y - t^6.621/y + (3*t^7.724)/y + (4*t^7.759)/y + (4*t^7.793)/y + (2*t^7.828)/y + t^7.862/y + t^8.862/y + (4*t^8.896)/y + (6*t^8.931)/y + t^8.965/y - t^4.207*y - t^6.552*y - 2*t^6.586*y - t^6.621*y + 3*t^7.724*y + 4*t^7.759*y + 4*t^7.793*y + 2*t^7.828*y + t^7.862*y + t^8.862*y + 4*t^8.896*y + 6*t^8.931*y + t^8.965*y g1^16*t^2.345 + 3*g1^6*t^2.379 + t^2.414/g1^4 + g1^24*t^3.517 + 2*g1^14*t^3.552 + g1^4*t^3.586 + g1^32*t^4.69 + 3*g1^22*t^4.724 + 7*g1^12*t^4.759 + 4*g1^2*t^4.793 + t^4.828/g1^8 + g1^40*t^5.862 + 5*g1^30*t^5.896 + 7*g1^20*t^5.931 + 3*g1^10*t^5.965 - 2*t^6. - (2*t^6.035)/g1^10 - t^6.069/g1^20 + 2*g1^48*t^7.034 + 5*g1^38*t^7.069 + 10*g1^28*t^7.103 + 13*g1^18*t^7.138 + 6*g1^8*t^7.172 - (2*t^7.241)/g1^12 - t^7.276/g1^22 + g1^56*t^8.207 + 5*g1^46*t^8.241 + 13*g1^36*t^8.276 + 15*g1^26*t^8.31 + 4*g1^16*t^8.345 - 9*g1^6*t^8.379 - (10*t^8.414)/g1^4 - (6*t^8.448)/g1^14 - t^8.483/g1^24 - t^4.207/(g1^2*y) - (g1^14*t^6.552)/y - (2*g1^4*t^6.586)/y - t^6.621/(g1^6*y) + (3*g1^22*t^7.724)/y + (4*g1^12*t^7.759)/y + (4*g1^2*t^7.793)/y + (2*t^7.828)/(g1^8*y) + t^7.862/(g1^18*y) + (g1^40*t^8.862)/y + (4*g1^30*t^8.896)/y + (6*g1^20*t^8.931)/y + (g1^10*t^8.965)/y - (t^4.207*y)/g1^2 - g1^14*t^6.552*y - 2*g1^4*t^6.586*y - (t^6.621*y)/g1^6 + 3*g1^22*t^7.724*y + 4*g1^12*t^7.759*y + 4*g1^2*t^7.793*y + (2*t^7.828*y)/g1^8 + (t^7.862*y)/g1^18 + g1^40*t^8.862*y + 4*g1^30*t^8.896*y + 6*g1^20*t^8.931*y + g1^10*t^8.965*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
1209 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{6}$ 0.6301 0.7812 0.8066 [M:[1.2032, 0.8075, 0.7968, 0.7968, 0.7914, 1.1925], q:[0.7995, 0.393], qb:[0.4038, 0.7995], phi:[0.4011]] t^2.374 + 2*t^2.39 + t^2.406 + t^3.561 + 2*t^3.577 + t^3.594 + t^3.61 + t^4.748 + 2*t^4.764 + 4*t^4.781 + 3*t^4.797 + t^4.813 + t^5.935 + 4*t^5.952 + 5*t^5.968 + 3*t^5.984 - t^4.203/y - t^4.203*y detail