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
1657 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ 0.6795 0.867 0.7837 [M:[0.8, 1.2, 0.8, 0.8, 0.8, 0.8, 0.8], q:[0.8, 0.4], qb:[0.8, 0.4], phi:[0.4]] [M:[[1], [0], [-1], [0], [0], [2], [-2]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] 1 {a: 1359/2000, c: 867/1000, M1: 4/5, M2: 6/5, M3: 4/5, M4: 4/5, M5: 4/5, M6: 4/5, M7: 4/5, q1: 4/5, q2: 2/5, qb1: 4/5, qb2: 2/5, phi1: 2/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{1}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{6}$, ${ }q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{3}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}^{2}$ ${}M_{3}q_{1}q_{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{6}q_{1}q_{2}$, ${ }M_{7}q_{1}q_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{7}q_{1}\tilde{q}_{2}$ 5 7*t^2.4 + 2*t^3.6 + 29*t^4.8 + 5*t^6. + 77*t^7.2 - 12*t^8.4 - t^4.2/y - (6*t^6.6)/y + (27*t^7.8)/y - t^4.2*y - 6*t^6.6*y + 27*t^7.8*y 3*t^2.4 + t^2.4/g1^2 + t^2.4/g1 + g1*t^2.4 + g1^2*t^2.4 + t^3.6/g1 + g1*t^3.6 + 9*t^4.8 + t^4.8/g1^4 + t^4.8/g1^3 + (4*t^4.8)/g1^2 + (4*t^4.8)/g1 + 4*g1*t^4.8 + 4*g1^2*t^4.8 + g1^3*t^4.8 + g1^4*t^4.8 - t^6. + t^6./g1^3 + (2*t^6.)/g1 + 2*g1*t^6. + g1^3*t^6. + 17*t^7.2 + t^7.2/g1^6 + t^7.2/g1^5 + (4*t^7.2)/g1^4 + (5*t^7.2)/g1^3 + (11*t^7.2)/g1^2 + (8*t^7.2)/g1 + 8*g1*t^7.2 + 11*g1^2*t^7.2 + 5*g1^3*t^7.2 + 4*g1^4*t^7.2 + g1^5*t^7.2 + g1^6*t^7.2 - 8*t^8.4 + t^8.4/g1^5 + (2*t^8.4)/g1^3 - (4*t^8.4)/g1^2 - t^8.4/g1 - g1*t^8.4 - 4*g1^2*t^8.4 + 2*g1^3*t^8.4 + g1^5*t^8.4 - t^4.2/y - (2*t^6.6)/y - t^6.6/(g1^2*y) - t^6.6/(g1*y) - (g1*t^6.6)/y - (g1^2*t^6.6)/y + (7*t^7.8)/y + t^7.8/(g1^3*y) + (4*t^7.8)/(g1^2*y) + (5*t^7.8)/(g1*y) + (5*g1*t^7.8)/y + (4*g1^2*t^7.8)/y + (g1^3*t^7.8)/y - t^4.2*y - 2*t^6.6*y - (t^6.6*y)/g1^2 - (t^6.6*y)/g1 - g1*t^6.6*y - g1^2*t^6.6*y + 7*t^7.8*y + (t^7.8*y)/g1^3 + (4*t^7.8*y)/g1^2 + (5*t^7.8*y)/g1 + 5*g1*t^7.8*y + 4*g1^2*t^7.8*y + g1^3*t^7.8*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
1063 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$ 0.7228 0.9222 0.7838 [M:[0.9709, 1.124, 0.9709, 0.6861, 0.876, 0.6861, 0.6861], q:[0.781, 0.438], qb:[0.5911, 0.438], phi:[0.438]] 3*t^2.058 + 2*t^2.628 + 2*t^2.913 + 2*t^3.657 + 7*t^4.116 + 2*t^4.401 + 6*t^4.686 + t^4.861 + 6*t^4.971 + 3*t^5.256 + 2*t^5.541 + 6*t^5.715 + 3*t^5.826 - 5*t^6. - t^4.314/y - t^4.314*y detail