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
1483 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}M_{6}$ 0.6937 0.8506 0.8156 [M:[0.9796, 1.0068, 1.0204, 0.966, 1.034, 0.966], q:[0.517, 0.5034], qb:[0.4626, 0.5306], phi:[0.4966]] [M:[[-6], [2], [6], [-10], [10], [-10]], q:[[5], [1]], qb:[[-11], [9]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{6}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}^{4}$ ${}$ -2 2*t^2.898 + t^2.939 + t^2.98 + t^3.02 + t^3.061 + t^3.143 + t^4.265 + t^4.388 + t^4.429 + t^4.469 + t^4.51 + t^4.551 + 2*t^4.592 + t^4.633 + t^4.673 + 2*t^5.796 + t^5.837 + 2*t^5.878 + 2*t^5.918 + 2*t^5.959 - 2*t^6. + t^6.041 + t^6.082 + t^6.122 + t^6.286 + 2*t^7.163 + t^7.204 + t^7.245 + t^7.286 + 2*t^7.327 + 2*t^7.367 + 3*t^7.408 + 2*t^7.449 + 2*t^7.49 + 2*t^7.531 + 4*t^7.571 + 2*t^7.612 + 2*t^7.653 + 2*t^7.735 + t^7.775 + t^7.816 + t^8.531 + t^8.653 + 3*t^8.694 + t^8.735 + 2*t^8.776 + 3*t^8.816 + 4*t^8.857 - 2*t^8.898 - 2*t^8.98 - t^4.49/y - t^7.388/y + t^7.592/y + t^8.796/y + (2*t^8.837)/y + (2*t^8.878)/y + (3*t^8.918)/y + (3*t^8.959)/y - t^4.49*y - t^7.388*y + t^7.592*y + t^8.796*y + 2*t^8.837*y + 2*t^8.878*y + 3*t^8.918*y + 3*t^8.959*y (2*t^2.898)/g1^10 + t^2.939/g1^6 + t^2.98/g1^2 + g1^2*t^3.02 + g1^6*t^3.061 + g1^14*t^3.143 + t^4.265/g1^23 + t^4.388/g1^11 + t^4.429/g1^7 + t^4.469/g1^3 + g1*t^4.51 + g1^5*t^4.551 + 2*g1^9*t^4.592 + g1^13*t^4.633 + g1^17*t^4.673 + (2*t^5.796)/g1^20 + t^5.837/g1^16 + (2*t^5.878)/g1^12 + (2*t^5.918)/g1^8 + (2*t^5.959)/g1^4 - 2*t^6. + g1^4*t^6.041 + g1^8*t^6.082 + g1^12*t^6.122 + g1^28*t^6.286 + (2*t^7.163)/g1^33 + t^7.204/g1^29 + t^7.245/g1^25 + t^7.286/g1^21 + (2*t^7.327)/g1^17 + (2*t^7.367)/g1^13 + (3*t^7.408)/g1^9 + (2*t^7.449)/g1^5 + (2*t^7.49)/g1 + 2*g1^3*t^7.531 + 4*g1^7*t^7.571 + 2*g1^11*t^7.612 + 2*g1^15*t^7.653 + 2*g1^23*t^7.735 + g1^27*t^7.775 + g1^31*t^7.816 + t^8.531/g1^46 + t^8.653/g1^34 + (3*t^8.694)/g1^30 + t^8.735/g1^26 + (2*t^8.776)/g1^22 + (3*t^8.816)/g1^18 + (4*t^8.857)/g1^14 - (2*t^8.898)/g1^10 - (2*t^8.98)/g1^2 - t^4.49/(g1*y) - t^7.388/(g1^11*y) + (g1^9*t^7.592)/y + t^8.796/(g1^20*y) + (2*t^8.837)/(g1^16*y) + (2*t^8.878)/(g1^12*y) + (3*t^8.918)/(g1^8*y) + (3*t^8.959)/(g1^4*y) - (t^4.49*y)/g1 - (t^7.388*y)/g1^11 + g1^9*t^7.592*y + (t^8.796*y)/g1^20 + (2*t^8.837*y)/g1^16 + (2*t^8.878*y)/g1^12 + (3*t^8.918*y)/g1^8 + (3*t^8.959*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
2591 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}M_{6}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ 0.5493 0.711 0.7725 [M:[0.8235, 1.0588, 1.1765, 0.7059, 1.2941, 0.7059], q:[0.6471, 0.5294], qb:[0.1765, 0.7647], phi:[0.4706]] 2*t^2.118 + 2*t^2.471 + t^2.824 + t^3.176 + 2*t^3.529 + t^3.882 + 4*t^4.235 + 4*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: 5397/9826, c: 13973/19652, M1: 14/17, M2: 18/17, M3: 20/17, M4: 12/17, M5: 22/17, M6: 12/17, q1: 11/17, q2: 9/17, qb1: 3/17, qb2: 13/17, 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
958 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ 0.6916 0.8474 0.8161 [M:[0.9938, 1.0021, 1.0062, 0.9897, 1.0103], q:[0.5051, 0.501], qb:[0.4887, 0.5092], phi:[0.499]] t^2.969 + t^2.982 + t^2.994 + t^3.006 + t^3.018 + t^3.031 + t^3.043 + t^4.429 + t^4.466 + t^4.478 + t^4.491 + t^4.503 + t^4.515 + 2*t^4.528 + t^4.54 + t^4.552 + t^5.963 + t^5.975 + t^5.988 - t^6. - t^4.497/y - t^4.497*y detail