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
45981 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ 0.5539 0.7073 0.7832 [M:[0.8693, 1.1307, 0.7198], q:[0.9882, 0.5772], qb:[0.2921, 0.4041], phi:[0.4346]] [M:[[-2, -2], [2, 2], [-9, -3]], q:[[6, 3], [-5, -2]], qb:[[3, 0], [0, 3]], phi:[[-1, -1]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ ${}M_{1}M_{2}$ -1 t^2.088 + t^2.159 + 2*t^2.608 + t^2.944 + t^3.056 + t^3.392 + t^3.728 + 2*t^4.177 + t^4.248 + t^4.319 + 3*t^4.696 + 2*t^4.767 + t^5.032 + t^5.103 + t^5.145 + 3*t^5.216 + t^5.481 + 2*t^5.552 + t^5.664 + t^5.817 + 2*t^5.888 - t^6. + t^6.112 + 2*t^6.265 + 3*t^6.336 + t^6.407 - t^6.448 + t^6.478 - t^6.519 + t^6.672 + 3*t^6.784 + 2*t^6.855 + 2*t^6.926 - t^6.968 + 2*t^7.12 + t^7.191 + t^7.233 + t^7.262 + 2*t^7.304 + 3*t^7.375 + t^7.456 + t^7.569 + t^7.64 + 2*t^7.711 + 3*t^7.823 + 2*t^7.905 + 2*t^7.976 + 2*t^8.047 - 3*t^8.088 - t^8.159 + t^8.201 + t^8.272 + 3*t^8.353 + 3*t^8.424 + 4*t^8.495 - 2*t^8.537 + t^8.566 - 5*t^8.608 + t^8.637 - t^8.679 + t^8.72 + t^8.76 + 2*t^8.831 + 3*t^8.873 - t^4.304/y - t^6.463/y - t^6.912/y + t^7.248/y + (3*t^7.696)/y + (2*t^7.767)/y + t^8.032/y + t^8.103/y + (2*t^8.145)/y + (2*t^8.216)/y + t^8.481/y + (3*t^8.552)/y - t^8.623/y + (2*t^8.664)/y + t^8.817/y + t^8.888/y - t^4.304*y - t^6.463*y - t^6.912*y + t^7.248*y + 3*t^7.696*y + 2*t^7.767*y + t^8.032*y + t^8.103*y + 2*t^8.145*y + 2*t^8.216*y + t^8.481*y + 3*t^8.552*y - t^8.623*y + 2*t^8.664*y + t^8.817*y + t^8.888*y g1^3*g2^3*t^2.088 + t^2.159/(g1^9*g2^3) + (2*t^2.608)/(g1^2*g2^2) + (g2*t^2.944)/g1^5 + (g1^5*t^3.056)/g2 + g1^2*g2^2*t^3.392 + (g2^5*t^3.728)/g1 + 2*g1^6*g2^6*t^4.177 + t^4.248/g1^6 + t^4.319/(g1^18*g2^6) + 3*g1*g2*t^4.696 + (2*t^4.767)/(g1^11*g2^5) + (g2^4*t^5.032)/g1^2 + t^5.103/(g1^14*g2^2) + g1^8*g2^2*t^5.145 + (3*t^5.216)/(g1^4*g2^4) + g1^5*g2^5*t^5.481 + (2*t^5.552)/(g1^7*g2) + (g1^3*t^5.664)/g2^3 + g1^2*g2^8*t^5.817 + (2*g2^2*t^5.888)/g1^10 - t^6. + (g1^10*t^6.112)/g2^2 + 2*g1^9*g2^9*t^6.265 + (3*g2^3*t^6.336)/g1^3 + t^6.407/(g1^15*g2^3) - g1^7*g2*t^6.448 + t^6.478/(g1^27*g2^9) - t^6.519/(g1^5*g2^5) + (g2^6*t^6.672)/g1^6 + 3*g1^4*g2^4*t^6.784 + (2*t^6.855)/(g1^8*g2^2) + (2*t^6.926)/(g1^20*g2^8) - (g1^2*t^6.968)/g2^4 + 2*g1*g2^7*t^7.12 + (g2*t^7.191)/g1^11 + g1^11*g2^5*t^7.233 + t^7.262/(g1^23*g2^5) + (2*t^7.304)/(g1*g2) + (3*t^7.375)/(g1^13*g2^7) + (g2^10*t^7.456)/g1^2 + g1^8*g2^8*t^7.569 + (g2^2*t^7.64)/g1^4 + (2*t^7.711)/(g1^16*g2^4) + (3*t^7.823)/(g1^6*g2^6) + 2*g1^5*g2^11*t^7.905 + (2*g2^5*t^7.976)/g1^7 + (2*t^8.047)/(g1^19*g2) - 3*g1^3*g2^3*t^8.088 - t^8.159/(g1^9*g2^3) + g1^13*g2*t^8.201 + (g1*t^8.272)/g2^5 + 3*g1^12*g2^12*t^8.353 + 3*g2^6*t^8.424 + (4*t^8.495)/g1^12 - 2*g1^10*g2^4*t^8.537 + t^8.566/(g1^24*g2^6) - (5*t^8.608)/(g1^2*g2^2) + t^8.637/(g1^36*g2^12) - t^8.679/(g1^14*g2^8) + (g1^8*t^8.72)/g2^4 + (g2^9*t^8.76)/g1^3 + (2*g2^3*t^8.831)/g1^15 + 3*g1^7*g2^7*t^8.873 - t^4.304/(g1*g2*y) - t^6.463/(g1^10*g2^4*y) - t^6.912/(g1^3*g2^3*y) + t^7.248/(g1^6*y) + (3*g1*g2*t^7.696)/y + (2*t^7.767)/(g1^11*g2^5*y) + (g2^4*t^8.032)/(g1^2*y) + t^8.103/(g1^14*g2^2*y) + (2*g1^8*g2^2*t^8.145)/y + (2*t^8.216)/(g1^4*g2^4*y) + (g1^5*g2^5*t^8.481)/y + (3*t^8.552)/(g1^7*g2*y) - t^8.623/(g1^19*g2^7*y) + (2*g1^3*t^8.664)/(g2^3*y) + (g1^2*g2^8*t^8.817)/y + (g2^2*t^8.888)/(g1^10*y) - (t^4.304*y)/(g1*g2) - (t^6.463*y)/(g1^10*g2^4) - (t^6.912*y)/(g1^3*g2^3) + (t^7.248*y)/g1^6 + 3*g1*g2*t^7.696*y + (2*t^7.767*y)/(g1^11*g2^5) + (g2^4*t^8.032*y)/g1^2 + (t^8.103*y)/(g1^14*g2^2) + 2*g1^8*g2^2*t^8.145*y + (2*t^8.216*y)/(g1^4*g2^4) + g1^5*g2^5*t^8.481*y + (3*t^8.552*y)/(g1^7*g2) - (t^8.623*y)/(g1^19*g2^7) + (2*g1^3*t^8.664*y)/g2^3 + g1^2*g2^8*t^8.817*y + (g2^2*t^8.888*y)/g1^10


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
45900 SU2adj1nf2 ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ 0.669 0.8356 0.8006 [M:[0.7, 0.6922, 0.6922], q:[0.825, 0.825], qb:[0.4828, 0.4672], phi:[0.35]] 2*t^2.077 + 2*t^2.1 + t^2.85 + t^3.853 + 2*t^3.877 + t^3.947 + 3*t^4.153 + 4*t^4.177 + 3*t^4.2 + 2*t^4.927 + 3*t^4.95 + t^5.7 + 2*t^5.93 + 5*t^5.953 + 2*t^5.977 - 3*t^6. - t^4.05/y - t^4.05*y detail