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
57605 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$ 1.3128 1.5628 0.84 [X:[], M:[], q:[0.56, 0.48], qb:[0.32, 0.24], phi:[0.4]] [X:[], M:[], q:[[-1], [2]], qb:[[-2], [1]], phi:[[0]]] 1 {a: 1641/1250, c: 3907/2500, q1: 14/25, q2: 12/25, qb1: 8/25, qb2: 6/25, phi1: 2/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{3}$ ${2}\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ 2}\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ 3}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ 2}\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ 2}\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ 12 t^2.16 + 3*t^2.4 + t^2.64 + t^3.36 + 4*t^3.6 + 2*t^3.84 + t^4.32 + 4*t^4.56 + 10*t^4.8 + 5*t^5.04 + t^5.28 + t^5.52 + 7*t^5.76 + 12*t^6. + 8*t^6.24 + 4*t^6.48 + 5*t^6.72 + 14*t^6.96 + 27*t^7.2 + 16*t^7.44 + 8*t^7.68 + 10*t^7.92 + 19*t^8.16 + 29*t^8.4 + 24*t^8.64 + 17*t^8.88 - t^4.2/y - t^5.4/y - t^6.36/y - (3*t^6.6)/y - t^6.84/y + (2*t^7.56)/y + t^7.8/y + (2*t^8.04)/y + (3*t^8.76)/y - t^4.2*y - t^5.4*y - t^6.36*y - 3*t^6.6*y - t^6.84*y + 2*t^7.56*y + t^7.8*y + 2*t^8.04*y + 3*t^8.76*y g1^3*t^2.16 + 3*t^2.4 + t^2.64/g1^3 + g1^3*t^3.36 + 4*t^3.6 + (2*t^3.84)/g1^3 + g1^6*t^4.32 + 4*g1^3*t^4.56 + 10*t^4.8 + (5*t^5.04)/g1^3 + t^5.28/g1^6 + g1^6*t^5.52 + 7*g1^3*t^5.76 + 12*t^6. + (8*t^6.24)/g1^3 + (3*t^6.48)/g1^6 + g1^9*t^6.48 + 5*g1^6*t^6.72 + 14*g1^3*t^6.96 + 27*t^7.2 + (16*t^7.44)/g1^3 + (7*t^7.68)/g1^6 + g1^9*t^7.68 + t^7.92/g1^9 + 9*g1^6*t^7.92 + 19*g1^3*t^8.16 + 29*t^8.4 + (23*t^8.64)/g1^3 + g1^12*t^8.64 + (12*t^8.88)/g1^6 + 5*g1^9*t^8.88 - t^4.2/y - t^5.4/y - (g1^3*t^6.36)/y - (3*t^6.6)/y - t^6.84/(g1^3*y) + (2*g1^3*t^7.56)/y + t^7.8/y + (2*t^8.04)/(g1^3*y) + (3*g1^3*t^8.76)/y - t^4.2*y - t^5.4*y - g1^3*t^6.36*y - 3*t^6.6*y - (t^6.84*y)/g1^3 + 2*g1^3*t^7.56*y + t^7.8*y + (2*t^8.04*y)/g1^3 + 3*g1^3*t^8.76*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


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
47927 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ 1.3249 1.5749 0.8413 [q:[0.5888, 0.4225], qb:[0.2944, 0.2944], phi:[0.4]] 2*t^2.151 + t^2.4 + 2*t^2.649 + 2*t^3.351 + t^3.6 + 4*t^3.849 + 3*t^4.301 + 4*t^4.551 + 5*t^4.8 + 6*t^5.049 + 3*t^5.299 + 4*t^5.501 + 4*t^5.751 + 7*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail