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
46554 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ 0.6383 0.8373 0.7623 [M:[0.9631, 0.7039, 0.8513, 0.8894], q:[0.7408, 0.2961], qb:[0.4816, 0.4079], phi:[0.5184]] [M:[[4], [5], [-11], [12]], q:[[1], [-5]], qb:[[2], [10]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{3}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{4}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ ${}$ -1 2*t^2.112 + t^2.333 + t^2.554 + 2*t^2.668 + t^2.889 + t^3.111 + 2*t^3.667 + t^4.003 + 4*t^4.224 + 3*t^4.445 + 3*t^4.666 + 4*t^4.78 + t^4.887 + 4*t^5.001 + t^5.108 + 5*t^5.222 + 3*t^5.337 + t^5.443 + 2*t^5.558 + 5*t^5.779 - t^6. + 2*t^6.114 + 9*t^6.335 + 5*t^6.557 + 2*t^6.671 + 5*t^6.778 + 8*t^6.892 + t^6.999 + 9*t^7.113 + 2*t^7.22 + 10*t^7.334 + t^7.441 + 6*t^7.448 + t^7.555 + t^7.662 + 8*t^7.67 + t^7.776 + 11*t^7.891 + 5*t^8.005 - 2*t^8.112 + 7*t^8.226 - 3*t^8.333 + 16*t^8.447 - 5*t^8.554 + 4*t^8.668 - t^8.775 + 4*t^8.783 + 3*t^8.889 - t^4.555/y - t^6.667/y - t^7.109/y + (2*t^7.445)/y + (2*t^7.666)/y + (4*t^7.78)/y + (2*t^7.887)/y + (5*t^8.001)/y + (5*t^8.222)/y + t^8.337/y + (3*t^8.443)/y + (2*t^8.558)/y + t^8.665/y + (5*t^8.779)/y - t^4.555*y - t^6.667*y - t^7.109*y + 2*t^7.445*y + 2*t^7.666*y + 4*t^7.78*y + 2*t^7.887*y + 5*t^8.001*y + 5*t^8.222*y + t^8.337*y + 3*t^8.443*y + 2*t^8.558*y + t^8.665*y + 5*t^8.779*y 2*g1^5*t^2.112 + t^2.333/g1^3 + t^2.554/g1^11 + 2*g1^12*t^2.668 + g1^4*t^2.889 + t^3.111/g1^4 + 2*g1^3*t^3.667 + g1^18*t^4.003 + 4*g1^10*t^4.224 + 3*g1^2*t^4.445 + (3*t^4.666)/g1^6 + 4*g1^17*t^4.78 + t^4.887/g1^14 + 4*g1^9*t^5.001 + t^5.108/g1^22 + 5*g1*t^5.222 + 3*g1^24*t^5.337 + t^5.443/g1^7 + 2*g1^16*t^5.558 + 5*g1^8*t^5.779 - t^6. + 2*g1^23*t^6.114 + 9*g1^15*t^6.335 + 5*g1^7*t^6.557 + 2*g1^30*t^6.671 + (5*t^6.778)/g1 + 8*g1^22*t^6.892 + t^6.999/g1^9 + 9*g1^14*t^7.113 + (2*t^7.22)/g1^17 + 10*g1^6*t^7.334 + t^7.441/g1^25 + 6*g1^29*t^7.448 + t^7.555/g1^2 + t^7.662/g1^33 + 8*g1^21*t^7.67 + t^7.776/g1^10 + 11*g1^13*t^7.891 + 5*g1^36*t^8.005 - 2*g1^5*t^8.112 + 7*g1^28*t^8.226 - (3*t^8.333)/g1^3 + 16*g1^20*t^8.447 - (5*t^8.554)/g1^11 + 4*g1^12*t^8.668 - t^8.775/g1^19 + 4*g1^35*t^8.783 + 3*g1^4*t^8.889 - t^4.555/(g1^2*y) - (g1^3*t^6.667)/y - t^7.109/(g1^13*y) + (2*g1^2*t^7.445)/y + (2*t^7.666)/(g1^6*y) + (4*g1^17*t^7.78)/y + (2*t^7.887)/(g1^14*y) + (5*g1^9*t^8.001)/y + (5*g1*t^8.222)/y + (g1^24*t^8.337)/y + (3*t^8.443)/(g1^7*y) + (2*g1^16*t^8.558)/y + t^8.665/(g1^15*y) + (5*g1^8*t^8.779)/y - (t^4.555*y)/g1^2 - g1^3*t^6.667*y - (t^7.109*y)/g1^13 + 2*g1^2*t^7.445*y + (2*t^7.666*y)/g1^6 + 4*g1^17*t^7.78*y + (2*t^7.887*y)/g1^14 + 5*g1^9*t^8.001*y + 5*g1*t^8.222*y + g1^24*t^8.337*y + (3*t^8.443*y)/g1^7 + 2*g1^16*t^8.558*y + (t^8.665*y)/g1^15 + 5*g1^8*t^8.779*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
47264 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ 0.656 0.8685 0.7554 [M:[0.9649, 0.7062, 0.8464, 0.8948, 0.7763], q:[0.7412, 0.2938], qb:[0.4825, 0.4123], phi:[0.5175]] 2*t^2.118 + 2*t^2.329 + t^2.539 + 2*t^2.684 + t^2.895 + t^3.105 + t^3.671 + t^4.027 + 4*t^4.237 + 5*t^4.447 + 5*t^4.658 + 4*t^4.803 + 2*t^4.868 + 6*t^5.013 + t^5.079 + 6*t^5.224 + 3*t^5.369 + 2*t^5.434 + 2*t^5.579 + 3*t^5.79 - t^6. - t^4.553/y - t^4.553*y detail


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
46257 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ 0.6298 0.8204 0.7677 [M:[0.9757, 0.7196, 0.8168], q:[0.7439, 0.2804], qb:[0.4879, 0.4393], phi:[0.5121]] 2*t^2.159 + t^2.305 + t^2.45 + t^2.781 + t^2.927 + t^3.073 + t^3.219 + 2*t^3.695 + t^4.172 + 4*t^4.318 + 3*t^4.464 + 3*t^4.609 + t^4.755 + t^4.901 + 2*t^4.94 + 3*t^5.086 + 4*t^5.232 + 3*t^5.378 + t^5.523 + t^5.563 + t^5.669 + t^5.708 + 4*t^5.854 - t^4.536/y - t^4.536*y detail