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
899 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ 0.702 0.8645 0.812 [M:[0.933, 1.0223, 1.067, 0.8883, 0.933], q:[0.4665, 0.6005], qb:[0.4665, 0.5112], phi:[0.4888]] [M:[[-6], [2], [6], [-10], [-6]], q:[[-3], [9]], qb:[[-3], [1]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ ${}$ -2 t^2.665 + 2*t^2.799 + 2*t^2.933 + t^3.067 + t^3.201 + 3*t^4.265 + 2*t^4.399 + t^4.534 + 2*t^4.668 + t^4.802 + t^5.07 + t^5.33 + 2*t^5.464 + 3*t^5.598 + 4*t^5.732 + 4*t^5.866 - 2*t^6. - t^6.402 + 3*t^6.93 + 6*t^7.064 + 8*t^7.198 + 5*t^7.332 + 3*t^7.466 + t^7.601 + t^7.735 + t^7.869 + t^7.995 + t^8.003 + 2*t^8.129 + 3*t^8.263 + t^8.271 + 5*t^8.397 + 10*t^8.531 + 4*t^8.665 - 2*t^8.799 - 3*t^8.933 - t^4.466/y - t^7.131/y - t^7.265/y + t^7.668/y + t^7.802/y + (2*t^8.464)/y + (3*t^8.598)/y + (5*t^8.732)/y + (4*t^8.866)/y - t^4.466*y - t^7.131*y - t^7.265*y + t^7.668*y + t^7.802*y + 2*t^8.464*y + 3*t^8.598*y + 5*t^8.732*y + 4*t^8.866*y t^2.665/g1^10 + (2*t^2.799)/g1^6 + (2*t^2.933)/g1^2 + g1^2*t^3.067 + g1^6*t^3.201 + (3*t^4.265)/g1^7 + (2*t^4.399)/g1^3 + g1*t^4.534 + 2*g1^5*t^4.668 + g1^9*t^4.802 + g1^17*t^5.07 + t^5.33/g1^20 + (2*t^5.464)/g1^16 + (3*t^5.598)/g1^12 + (4*t^5.732)/g1^8 + (4*t^5.866)/g1^4 - 2*t^6. - g1^12*t^6.402 + (3*t^6.93)/g1^17 + (6*t^7.064)/g1^13 + (8*t^7.198)/g1^9 + (5*t^7.332)/g1^5 + (3*t^7.466)/g1 + g1^3*t^7.601 + g1^7*t^7.735 + g1^11*t^7.869 + t^7.995/g1^30 + g1^15*t^8.003 + (2*t^8.129)/g1^26 + (3*t^8.263)/g1^22 + g1^23*t^8.271 + (5*t^8.397)/g1^18 + (10*t^8.531)/g1^14 + (4*t^8.665)/g1^10 - (2*t^8.799)/g1^6 - (3*t^8.933)/g1^2 - t^4.466/(g1*y) - t^7.131/(g1^11*y) - t^7.265/(g1^7*y) + (g1^5*t^7.668)/y + (g1^9*t^7.802)/y + (2*t^8.464)/(g1^16*y) + (3*t^8.598)/(g1^12*y) + (5*t^8.732)/(g1^8*y) + (4*t^8.866)/(g1^4*y) - (t^4.466*y)/g1 - (t^7.131*y)/g1^11 - (t^7.265*y)/g1^7 + g1^5*t^7.668*y + g1^9*t^7.802*y + (2*t^8.464*y)/g1^16 + (3*t^8.598*y)/g1^12 + (5*t^8.732*y)/g1^8 + (4*t^8.866*y)/g1^4


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
1385 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{6}$ 0.7042 0.8689 0.8105 [M:[0.9263, 1.0246, 1.0737, 0.8772, 0.9263, 0.9754], q:[0.4632, 0.6105], qb:[0.4632, 0.5123], phi:[0.4877]] t^2.632 + 2*t^2.779 + 3*t^2.926 + t^3.221 + 3*t^4.242 + 2*t^4.39 + t^4.537 + 2*t^4.684 + t^4.831 + t^5.126 + t^5.263 + 2*t^5.411 + 4*t^5.558 + 5*t^5.705 + 5*t^5.853 - 4*t^6. - t^4.463/y - t^4.463*y detail
1383 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ 0.6942 0.85 0.8166 [M:[0.9652, 1.0116, 1.0348, 0.942, 0.9652, 1.058], q:[0.4826, 0.5522], qb:[0.4826, 0.5058], phi:[0.4942]] 2*t^2.896 + 2*t^2.965 + t^3.035 + t^3.104 + t^3.174 + 3*t^4.378 + 2*t^4.448 + t^4.517 + 2*t^4.587 + t^4.657 + t^4.796 + t^5.791 + 3*t^5.861 + 3*t^5.93 - 2*t^6. - t^4.483/y - t^4.483*y detail
1384 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}^{2}$ 0.7 0.8606 0.8133 [M:[0.9396, 1.0201, 1.0604, 0.8994, 0.9396, 1.0201], q:[0.4698, 0.5906], qb:[0.4698, 0.5101], phi:[0.4899]] t^2.698 + 2*t^2.819 + t^2.94 + 2*t^3.06 + t^3.181 + 3*t^4.289 + 2*t^4.409 + t^4.53 + 2*t^4.651 + t^4.772 + t^5.013 + t^5.396 + 2*t^5.517 + 2*t^5.638 + 3*t^5.758 + 4*t^5.879 - 2*t^6. - t^4.47/y - t^4.47*y detail
2083 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ 0.709 0.8787 0.8069 [M:[0.9142, 1.0286, 1.0858, 0.8571, 0.9142, 0.9142], q:[0.4571, 0.6286], qb:[0.4571, 0.5143], phi:[0.4857]] t^2.571 + 3*t^2.743 + 2*t^2.914 + t^3.086 + 3*t^4.2 + 2*t^4.371 + t^4.543 + 2*t^4.714 + t^4.886 + t^5.142 + t^5.229 + 3*t^5.314 + 6*t^5.485 + 6*t^5.657 + 4*t^5.828 - 4*t^6. - t^4.457/y - t^4.457*y detail
2081 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}^{2}$ 0.6742 0.847 0.796 [M:[0.8235, 1.0588, 1.1765, 0.7059, 0.8235], q:[0.4118, 0.7647], qb:[0.4118, 0.5294], phi:[0.4706]] t^2.118 + 2*t^2.471 + 2*t^2.824 + t^3.176 + t^3.529 + 3*t^3.882 + 3*t^4.235 + 3*t^4.588 + 5*t^4.941 + 5*t^5.294 + 4*t^5.647 + 2*t^6. - t^4.412/y - t^4.412*y detail {a: 52995/78608, c: 33289/39304, M1: 14/17, M2: 18/17, M3: 20/17, M4: 12/17, M5: 14/17, q1: 7/17, q2: 13/17, qb1: 7/17, qb2: 9/17, phi1: 8/17}


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
580 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ 0.7035 0.8668 0.8116 [M:[0.9248, 1.0251, 1.0752, 0.8746, 0.9248], q:[0.4849, 0.5904], qb:[0.4399, 0.535], phi:[0.4875]] t^2.624 + 2*t^2.774 + t^2.925 + t^3.06 + t^3.075 + t^3.091 + t^4.102 + t^4.237 + t^4.372 + t^4.387 + t^4.522 + t^4.553 + t^4.673 + t^4.688 + t^4.839 + t^5.005 + t^5.248 + 2*t^5.398 + 3*t^5.549 + 3*t^5.699 + t^5.834 + 2*t^5.85 + t^5.865 + t^5.985 - 3*t^6. - t^4.462/y - t^4.462*y detail