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
45792 SU3adj1nf1 $\phi_1^2X_1$ + $ \phi_1^3X_2$ + $ M_1\phi_1q_1\tilde{q}_1$ + $ M_2\phi_1^2q_1\tilde{q}_1$ + $ M_1M_2$ + $ q_1\tilde{q}_1X_3$ + $ M_1M_3$ 0.8642 0.9336 0.9256 [X:[1.5556, 1.3333, 1.3333], M:[1.1111, 0.8889, 0.8889], q:[0.3333], qb:[0.3333], phi:[0.2222]] [X:[[0], [0], [0]], M:[[0], [0], [0]], q:[[-1]], qb:[[1]], phi:[[0]]] 1 {a: 70/81, c: 605/648, X1: 14/9, X2: 4/3, X3: 4/3, M1: 10/9, M2: 8/9, M3: 8/9, q1: 1/3, qb1: 1/3, phi1: 2/9}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_2$, $ M_3$, $ X_2$, $ X_3$, $ X_1$, $ \phi_1^3q_1^3$, $ \phi_1^3\tilde{q}_1^3$, $ M_2^2$, $ M_2M_3$, $ M_3^2$ . -2 2*t^2.67 + 2*t^4. + t^4.67 + 2*t^5. + 3*t^5.33 - 2*t^6. + 3*t^6.67 + t^7.33 + 2*t^7.67 + 7*t^8. - 2*t^8.33 - 2*t^8.67 + t^8./y^2 - t^3.67/y - t^4.33/y - t^6.33/y - t^7./y - t^7.67/y - t^8.33/y - t^3.67*y - t^4.33*y - t^6.33*y - t^7.*y - t^7.67*y - t^8.33*y + t^8.*y^2 2*t^2.67 + 2*t^4. + t^4.67 + t^5./g1^3 + g1^3*t^5. + 3*t^5.33 - 2*t^6. + 3*t^6.67 + t^7.33 + t^7.67/g1^3 + g1^3*t^7.67 + 7*t^8. - t^8.33/g1^3 - g1^3*t^8.33 - 2*t^8.67 + t^8./y^2 - t^3.67/y - t^4.33/y - t^6.33/y - t^7./y - t^7.67/y - t^8.33/y - t^3.67*y - t^4.33*y - t^6.33*y - t^7.*y - t^7.67*y - t^8.33*y + t^8.*y^2


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
45794 $\phi_1^2X_1$ + $ \phi_1^3X_2$ + $ M_1\phi_1q_1\tilde{q}_1$ + $ M_2\phi_1^2q_1\tilde{q}_1$ + $ M_1M_2$ + $ q_1\tilde{q}_1X_3$ + $ M_1M_3$ + $ \phi_1^3\tilde{q}_1^3$ 0.8225 0.892 0.9221 [X:[1.5556, 1.3333, 1.3333], M:[1.1111, 0.8889, 0.8889], q:[0.2222], qb:[0.4444], phi:[0.2222]] 2*t^2.67 + 3*t^4. + t^4.67 + 3*t^5.33 - t^6. - t^3.67/y - t^4.33/y - t^3.67*y - t^4.33*y detail {a: 533/648, c: 289/324, X1: 14/9, X2: 4/3, X3: 4/3, M1: 10/9, M2: 8/9, M3: 8/9, q1: 2/9, qb1: 4/9, phi1: 2/9}


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
45784 SU3adj1nf1 $\phi_1^2X_1$ + $ \phi_1^3X_2$ + $ M_1\phi_1q_1\tilde{q}_1$ + $ M_2\phi_1^2q_1\tilde{q}_1$ + $ M_1M_2$ + $ q_1\tilde{q}_1X_3$ 0.8542 0.9167 0.9318 [X:[1.5556, 1.3333, 1.3333], M:[1.1111, 0.8889], q:[0.3333], qb:[0.3333], phi:[0.2222]] t^2.67 + t^3.33 + 2*t^4. + t^4.67 + 2*t^5. + t^5.33 - t^6. - t^3.67/y - t^4.33/y - t^3.67*y - t^4.33*y detail {a: 41/48, c: 11/12, X1: 14/9, X2: 4/3, X3: 4/3, M1: 10/9, M2: 8/9, q1: 1/3, qb1: 1/3, phi1: 2/9}