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
58431 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{1}^{2}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ 1.3244 1.5494 0.8548 [X:[1.4], M:[1.0], q:[0.2848, 0.4576], qb:[0.3152, 0.5424], phi:[0.4]] [X:[[0]], M:[[0]], q:[[2], [-1]], qb:[[-2], [1]], phi:[[0]]] 1 {a: 233091/176000, c: 272691/176000, X1: 7/5, M1: 1, q1: 47/165, q2: 151/330, qb1: 52/165, qb2: 179/330, phi1: 2/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ ${}M_{1}q_{2}\tilde{q}_{2}$, ${ 2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ 3 t^2.32 + t^2.4 + t^2.48 + 2*t^3. + t^3.52 + t^3.6 + t^3.68 + 3*t^4.2 + t^4.28 + t^4.64 + 3*t^4.72 + 3*t^4.8 + 2*t^4.88 + t^4.96 + t^5.32 + 4*t^5.4 + 2*t^5.48 + t^5.84 + 3*t^5.92 + 3*t^6. + 2*t^6.08 + 2*t^6.16 + t^6.44 + 3*t^6.52 + 5*t^6.6 + 5*t^6.68 + t^6.76 + t^6.95 + 4*t^7.04 + 6*t^7.12 + 10*t^7.2 + 4*t^7.28 + 3*t^7.36 + t^7.45 + t^7.64 + 7*t^7.72 + 7*t^7.8 + 7*t^7.88 + 2*t^7.96 + t^8.15 + 4*t^8.24 + 3*t^8.32 + 12*t^8.4 + 5*t^8.48 + 4*t^8.56 + 2*t^8.65 + t^8.75 + 2*t^8.84 + 9*t^8.92 - t^4.2/y - t^5.4/y - t^6.52/y - t^6.6/y - t^6.68/y - t^7.2/y + (2*t^8.32)/y - t^8.4/y + (2*t^8.48)/y - t^4.2*y - t^5.4*y - t^6.52*y - t^6.6*y - t^6.68*y - t^7.2*y + 2*t^8.32*y - t^8.4*y + 2*t^8.48*y t^2.32/g1^3 + t^2.4 + g1^3*t^2.48 + 2*t^3. + t^3.52/g1^3 + t^3.6 + g1^3*t^3.68 + 3*t^4.2 + g1^3*t^4.28 + t^4.64/g1^6 + (3*t^4.72)/g1^3 + 3*t^4.8 + 2*g1^3*t^4.88 + g1^6*t^4.96 + t^5.32/g1^3 + 4*t^5.4 + 2*g1^3*t^5.48 + t^5.84/g1^6 + (3*t^5.92)/g1^3 + 3*t^6. + 2*g1^3*t^6.08 + 2*g1^6*t^6.16 + t^6.44/g1^6 + (3*t^6.52)/g1^3 + 5*t^6.6 + 5*g1^3*t^6.68 + g1^6*t^6.76 + t^6.95/g1^9 + (4*t^7.04)/g1^6 + (6*t^7.12)/g1^3 + 10*t^7.2 + 4*g1^3*t^7.28 + 3*g1^6*t^7.36 + g1^9*t^7.45 + t^7.64/g1^6 + (7*t^7.72)/g1^3 + 7*t^7.8 + 7*g1^3*t^7.88 + 2*g1^6*t^7.96 + t^8.15/g1^9 + (4*t^8.24)/g1^6 + (3*t^8.32)/g1^3 + 12*t^8.4 + 5*g1^3*t^8.48 + 4*g1^6*t^8.56 + 2*g1^9*t^8.65 + t^8.75/g1^9 + (2*t^8.84)/g1^6 + (9*t^8.92)/g1^3 - t^4.2/y - t^5.4/y - t^6.52/(g1^3*y) - t^6.6/y - (g1^3*t^6.68)/y - t^7.2/y + (2*t^8.32)/(g1^3*y) - t^8.4/y + (2*g1^3*t^8.48)/y - t^4.2*y - t^5.4*y - (t^6.52*y)/g1^3 - t^6.6*y - g1^3*t^6.68*y - t^7.2*y + (2*t^8.32*y)/g1^3 - t^8.4*y + 2*g1^3*t^8.48*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
57351 SU3adj1nf2 ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ 1.427 1.6905 0.8441 [M:[0.7838], q:[0.4098, 0.3951], qb:[0.4065, 0.3887], phi:[0.4]] 2*t^2.351 + t^2.395 + t^2.4 + t^2.405 + t^2.449 + t^3.551 + t^3.595 + t^3.6 + t^3.605 + 3*t^4.703 + 2*t^4.747 + 4*t^4.751 + 2*t^4.756 + t^4.791 + 2*t^4.795 + 5*t^4.8 + 3*t^4.805 + t^4.809 + 2*t^4.844 + 2*t^4.849 + t^4.853 + t^4.897 + 2*t^5.903 + 2*t^5.947 + 4*t^5.951 + 2*t^5.956 + t^5.991 + 2*t^5.995 + t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y detail