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
98 SU2adj1nf2 $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ q_1\tilde{q}_1$ + $ \phi_1^2X_1$ + $ M_1\phi_1\tilde{q}_2^2$ 0.3583 0.3667 0.9773 [X:[1.7333], M:[0.8], q:[0.9333, 0.9333], qb:[1.0667, 0.5333], phi:[0.1333]] [X:[[4]], M:[[-12]], q:[[1], [1]], qb:[[-1], [7]], phi:[[-2]]] 1 {a: 43/120, c: 11/30, X1: 26/15, M1: 4/5, q1: 14/15, q2: 14/15, qb1: 16/15, qb2: 8/15, phi1: 2/15}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ q_2\tilde{q}_2$, $ M_1^2$ $q_2\tilde{q}_1$ -1 t^2.4 + t^4.4 + t^4.8 - t^6. + t^6.8 + t^7.2 + t^8. - t^8.4 - t^8.8 - t^8.8/y^2 - t^3.4/y - t^5.8/y + t^7./y - t^8.2/y - t^3.4*y - t^5.8*y + t^7.*y - t^8.2*y - t^8.8*y^2 t^2.4/g1^12 + g1^8*t^4.4 + t^4.8/g1^24 - t^6. + t^6.8/g1^4 + t^7.2/g1^36 + t^8./g1^10 - t^8.4/g1^12 - t^8.8/g1^14 - t^8.8/(g1^14*y^2) - t^3.4/(g1^2*y) - t^5.8/(g1^14*y) + (g1^10*t^7.)/y - t^8.2/(g1^26*y) - (t^3.4*y)/g1^2 - (t^5.8*y)/g1^14 + g1^10*t^7.*y - (t^8.2*y)/g1^26 - (t^8.8*y^2)/g1^14


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
155 $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ q_1\tilde{q}_1$ + $ \phi_1^2X_1$ + $ M_1\phi_1\tilde{q}_2^2$ + $ M_1^2$ 0.3424 0.3529 0.9705 [X:[1.6667], M:[1.0], q:[0.9167, 0.9167], qb:[1.0833, 0.4167], phi:[0.1667]] t^3. + t^4. - t^3.5/y - t^3.5*y detail {a: 263/768, c: 271/768, X1: 5/3, M1: 1, q1: 11/12, q2: 11/12, qb1: 13/12, qb2: 5/12, phi1: 1/6}


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
9 SU2adj1nf1 $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ \phi_1\tilde{q}_1^2$ 0.3583 0.3667 0.9773 [X:[1.7333], M:[0.8], q:[0.5333], qb:[0.9333], phi:[0.1333]] t^2.4 + t^4.4 + t^4.8 - t^6. - t^3.4/y - t^5.8/y - t^3.4*y - t^5.8*y detail {a: 43/120, c: 11/30, X1: 26/15, M1: 4/5, q1: 8/15, qb1: 14/15, phi1: 2/15}


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
62 SU2adj1nf2 $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ q_1\tilde{q}_1$ + $ \phi_1^2X_1$ 0.3451 0.3488 0.9895 [X:[1.6976], M:[], q:[0.9244, 0.9244], qb:[1.0756, 0.4708], phi:[0.1512]] t^3.28 + t^4.19 - t^6. - t^3.45/y - t^3.45*y detail