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
50970 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}$ 0.6633 0.8389 0.7907 [M:[0.8093, 0.7907, 1.2, 0.8, 0.8093, 0.7814], q:[0.8, 0.3907], qb:[0.4093, 0.8], phi:[0.4]] [M:[[1], [-1], [0], [0], [1], [-2]], q:[[0], [-1]], qb:[[1], [0]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{6}$, ${ }M_{2}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}M_{2}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ ${}M_{3}M_{4}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ 0 t^2.344 + t^2.372 + 2*t^2.4 + 2*t^2.428 + t^3.544 + t^3.6 + t^3.628 + t^4.689 + t^4.717 + 3*t^4.744 + 4*t^4.772 + 6*t^4.8 + 4*t^4.828 + 3*t^4.856 + t^5.889 + t^5.917 + 2*t^5.944 + 2*t^5.972 + 2*t^6.028 + t^6.056 + t^7.033 + t^7.061 + 4*t^7.089 + 5*t^7.117 + 7*t^7.144 + 7*t^7.172 + 9*t^7.2 + 8*t^7.228 + 5*t^7.256 + 4*t^7.283 + t^8.233 + t^8.261 + 3*t^8.289 + 3*t^8.317 + 2*t^8.344 - 2*t^8.372 - t^8.4 - 3*t^8.428 + t^8.483 - t^4.2/y - t^6.544/y - t^6.572/y - t^6.6/y - (2*t^6.628)/y + t^7.717/y + (2*t^7.744)/y + (6*t^7.772)/y + (4*t^7.8)/y + (5*t^7.828)/y + (2*t^7.856)/y + t^8.944/y + t^8.972/y - t^4.2*y - t^6.544*y - t^6.572*y - t^6.6*y - 2*t^6.628*y + t^7.717*y + 2*t^7.744*y + 6*t^7.772*y + 4*t^7.8*y + 5*t^7.828*y + 2*t^7.856*y + t^8.944*y + t^8.972*y t^2.344/g1^2 + t^2.372/g1 + 2*t^2.4 + 2*g1*t^2.428 + t^3.544/g1^2 + t^3.6 + g1*t^3.628 + t^4.689/g1^4 + t^4.717/g1^3 + (3*t^4.744)/g1^2 + (4*t^4.772)/g1 + 6*t^4.8 + 4*g1*t^4.828 + 3*g1^2*t^4.856 + t^5.889/g1^4 + t^5.917/g1^3 + (2*t^5.944)/g1^2 + (2*t^5.972)/g1 + 2*g1*t^6.028 + g1^2*t^6.056 + t^7.033/g1^6 + t^7.061/g1^5 + (4*t^7.089)/g1^4 + (5*t^7.117)/g1^3 + (7*t^7.144)/g1^2 + (7*t^7.172)/g1 + 9*t^7.2 + 8*g1*t^7.228 + 5*g1^2*t^7.256 + 4*g1^3*t^7.283 + t^8.233/g1^6 + t^8.261/g1^5 + (3*t^8.289)/g1^4 + (3*t^8.317)/g1^3 + (2*t^8.344)/g1^2 - (2*t^8.372)/g1 - t^8.4 - 3*g1*t^8.428 + g1^3*t^8.483 - t^4.2/y - t^6.544/(g1^2*y) - t^6.572/(g1*y) - t^6.6/y - (2*g1*t^6.628)/y + t^7.717/(g1^3*y) + (2*t^7.744)/(g1^2*y) + (6*t^7.772)/(g1*y) + (4*t^7.8)/y + (5*g1*t^7.828)/y + (2*g1^2*t^7.856)/y + t^8.944/(g1^2*y) + t^8.972/(g1*y) - t^4.2*y - (t^6.544*y)/g1^2 - (t^6.572*y)/g1 - t^6.6*y - 2*g1*t^6.628*y + (t^7.717*y)/g1^3 + (2*t^7.744*y)/g1^2 + (6*t^7.772*y)/g1 + 4*t^7.8*y + 5*g1*t^7.828*y + 2*g1^2*t^7.856*y + (t^8.944*y)/g1^2 + (t^8.972*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
56227 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{6}^{2}$ 0.6269 0.7957 0.7879 [M:[0.7, 0.9, 1.2, 0.8, 0.7, 1.0], q:[0.8, 0.5], qb:[0.3, 0.8], phi:[0.4]] 2*t^2.1 + 2*t^2.4 + t^2.7 + t^3. + t^3.3 + t^3.6 + 4*t^4.2 + 4*t^4.5 + 6*t^4.8 + 4*t^5.1 + 4*t^5.4 + 3*t^5.7 + t^6. - t^4.2/y - t^4.2*y detail {a: 20061/32000, c: 25461/32000, M1: 7/10, M2: 9/10, M3: 6/5, M4: 4/5, M5: 7/10, M6: 1, q1: 4/5, q2: 1/2, qb1: 3/10, qb2: 4/5, phi1: 2/5}
56308 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ 0.6797 0.8677 0.7834 [M:[0.7923, 0.8077, 1.2, 0.8, 0.7923, 0.8154, 0.7846], q:[0.8, 0.4077], qb:[0.3923, 0.8], phi:[0.4]] t^2.354 + 2*t^2.377 + 2*t^2.4 + t^2.423 + t^2.446 + t^3.577 + t^3.6 + t^4.707 + 2*t^4.73 + 5*t^4.754 + 5*t^4.777 + 7*t^4.8 + 4*t^4.823 + 3*t^4.846 + t^4.87 + t^4.893 + t^5.93 + 2*t^5.954 + 2*t^5.977 - t^4.2/y - t^4.2*y detail


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
46946 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ 0.7089 0.895 0.7921 [M:[0.9777, 0.9907, 1.1181, 0.6772, 0.7731, 0.6902], q:[0.5749, 0.4474], qb:[0.4345, 0.7795], phi:[0.4409]] t^2.032 + t^2.071 + t^2.319 + t^2.646 + t^2.933 + t^2.972 + t^3.354 + t^3.642 + t^4.007 + 2*t^4.063 + t^4.102 + t^4.141 + 2*t^4.351 + 2*t^4.39 + t^4.638 + t^4.677 + t^4.716 + t^4.772 + 2*t^4.965 + 2*t^5.004 + t^5.042 + t^5.252 + 2*t^5.291 + t^5.386 + t^5.425 + 2*t^5.674 + t^5.712 + t^5.866 + t^5.905 + t^5.944 - 2*t^6. - t^4.323/y - t^4.323*y detail