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
59396 SU3adj1nf2 ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{1}M_{2}$ 1.4293 1.6637 0.8591 [X:[], M:[0.875, 1.125], q:[0.5, 0.375], qb:[0.5, 0.375], phi:[0.375]] [X:[], M:[[0, 0], [0, 0]], q:[[-1, 0], [0, -1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] 2 {a: 11709/8192, c: 13629/8192, M1: 7/8, M2: 9/8, q1: 1/2, q2: 3/8, qb1: 1/2, qb2: 3/8, phi1: 3/8}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{5}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ ${}\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ 2}\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ 2}\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ 7 2*t^2.25 + 2*t^2.62 + t^3. + 2*t^3.38 + 2*t^3.75 + t^4.12 + 4*t^4.5 + 8*t^4.88 + 8*t^5.25 + 4*t^5.62 + 7*t^6. + 8*t^6.38 + 13*t^6.75 + 17*t^7.12 + 24*t^7.5 + 21*t^7.88 + 16*t^8.25 + 17*t^8.62 - t^4.12/y - t^5.25/y - (2*t^6.38)/y - (2*t^6.75)/y - t^7.12/y - (2*t^7.5)/y + (3*t^7.88)/y + (2*t^8.25)/y + t^8.62/y - t^4.12*y - t^5.25*y - 2*t^6.38*y - 2*t^6.75*y - t^7.12*y - 2*t^7.5*y + 3*t^7.88*y + 2*t^8.25*y + t^8.62*y 2*t^2.25 + (g1*t^2.62)/g2 + (g2*t^2.62)/g1 + t^3. + 2*t^3.38 + (g1*t^3.75)/g2 + (g2*t^3.75)/g1 + t^4.12 + 4*t^4.5 + t^4.88/(g1*g2^2) + (3*g1*t^4.88)/g2 + (3*g2*t^4.88)/g1 + g1*g2^2*t^4.88 + 4*t^5.25 + (g1^2*t^5.25)/g2^2 + t^5.25/(g1^2*g2) + g1^2*g2*t^5.25 + (g2^2*t^5.25)/g1^2 + 4*t^5.62 - 3*t^6. + t^6./(g1*g2^2) + (4*g1*t^6.)/g2 + (4*g2*t^6.)/g1 + g1*g2^2*t^6. + 6*t^6.38 + (g1^2*t^6.38)/g2^2 + t^6.38/(g1^2*g2) - (g1*t^6.38)/g2 - (g2*t^6.38)/g1 + g1^2*g2*t^6.38 + (g2^2*t^6.38)/g1^2 + 9*t^6.75 + t^6.75/g2^3 + (g1*t^6.75)/g2 + (g2*t^6.75)/g1 + g2^3*t^6.75 - 3*t^7.12 + (3*t^7.12)/(g1*g2^2) - t^7.12/(g1^2*g2) + (8*g1*t^7.12)/g2 + (8*g2*t^7.12)/g1 - g1^2*g2*t^7.12 + 3*g1*g2^2*t^7.12 + 12*t^7.5 + t^7.5/g2^3 - t^7.5/(g1*g2^2) + (4*g1^2*t^7.5)/g2^2 + (4*t^7.5)/(g1^2*g2) - (2*g1*t^7.5)/g2 - (2*g2*t^7.5)/g1 + 4*g1^2*g2*t^7.5 + (4*g2^2*t^7.5)/g1^2 - g1*g2^2*t^7.5 + g2^3*t^7.5 + 7*t^7.88 + (2*t^7.88)/g1^3 + 2*g1^3*t^7.88 + (g1^3*t^7.88)/g2^3 + t^7.88/(g1*g2^2) + (3*g1*t^7.88)/g2 + (3*g2*t^7.88)/g1 + g1*g2^2*t^7.88 + (g2^3*t^7.88)/g1^3 - 8*t^8.25 - t^8.25/g2^3 + (4*t^8.25)/(g1*g2^2) - t^8.25/(g1^2*g2) + (10*g1*t^8.25)/g2 + (10*g2*t^8.25)/g1 - g1^2*g2*t^8.25 + 4*g1*g2^2*t^8.25 - g2^3*t^8.25 + 17*t^8.62 - t^8.62/g1^3 - g1^3*t^8.62 + (2*t^8.62)/g2^3 - (3*t^8.62)/(g1*g2^2) + (5*g1^2*t^8.62)/g2^2 + (5*t^8.62)/(g1^2*g2) - (8*g1*t^8.62)/g2 - (8*g2*t^8.62)/g1 + 5*g1^2*g2*t^8.62 + (5*g2^2*t^8.62)/g1^2 - 3*g1*g2^2*t^8.62 + 2*g2^3*t^8.62 - t^4.12/y - t^5.25/y - (2*t^6.38)/y - (g1*t^6.75)/(g2*y) - (g2*t^6.75)/(g1*y) - t^7.12/y - (2*t^7.5)/y + t^7.88/y + (g1*t^7.88)/(g2*y) + (g2*t^7.88)/(g1*y) + (2*t^8.25)/y - t^8.62/y + (g1*t^8.62)/(g2*y) + (g2*t^8.62)/(g1*y) - t^4.12*y - t^5.25*y - 2*t^6.38*y - (g1*t^6.75*y)/g2 - (g2*t^6.75*y)/g1 - t^7.12*y - 2*t^7.5*y + t^7.88*y + (g1*t^7.88*y)/g2 + (g2*t^7.88*y)/g1 + 2*t^8.25*y - t^8.62*y + (g1*t^8.62*y)/g2 + (g2*t^8.62*y)/g1


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
57471 SU3adj1nf2 ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ 1.4405 1.6827 0.8561 [X:[], M:[0.875], q:[0.5, 0.375], qb:[0.5, 0.375], phi:[0.375]] 2*t^2.25 + 3*t^2.62 + t^3. + t^3.38 + 2*t^3.75 + t^4.12 + 4*t^4.5 + 10*t^4.88 + 11*t^5.25 + 3*t^5.62 + 6*t^6. - t^4.12/y - t^5.25/y - t^4.12*y - t^5.25*y detail {a: 23601/16384, c: 27569/16384, M1: 7/8, q1: 1/2, q2: 3/8, qb1: 1/2, qb2: 3/8, phi1: 3/8}