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
624 SU2adj1nf2 $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4\phi_1^2$ 0.5267 0.6233 0.845 [X:[1.6364], M:[0.9091, 0.3636, 1.0909, 1.2727], q:[0.8182, 0.8182], qb:[0.2727, 0.6364], phi:[0.3636]] [X:[[0]], M:[[0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 11217/21296, c: 6637/10648, X1: 18/11, M1: 10/11, M2: 4/11, M3: 12/11, M4: 14/11, q1: 9/11, q2: 9/11, qb1: 3/11, qb2: 7/11, phi1: 4/11}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ \tilde{q}_1\tilde{q}_2$, $ M_3$, $ q_2\tilde{q}_1$, $ M_4$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ q_1q_2$, $ X_1$, $ M_1^2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$ $M_1q_2\tilde{q}_1$, $ q_2\tilde{q}_1^2\tilde{q}_2$ 0 2*t^2.73 + 2*t^3.27 + 2*t^3.82 + 2*t^4.36 + t^4.91 + t^5.45 + 2*t^6.55 + 3*t^7.09 + 3*t^7.64 + 3*t^8.18 - t^4.09/y + t^8.45/y - t^4.09*y + t^8.45*y 2*t^2.73 + 2*t^3.27 + 2*t^3.82 + 2*t^4.36 + t^4.91 + t^5.45 + 2*t^6.55 + 3*t^7.09 + 3*t^7.64 + 3*t^8.18 - t^4.09/y + t^8.45/y - t^4.09*y + t^8.45*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
384 SU2adj1nf2 $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ 0.5466 0.6602 0.8279 [X:[1.6364], M:[0.9091, 0.3636, 1.0909], q:[0.8182, 0.8182], qb:[0.2727, 0.6364], phi:[0.3636]] t^2.18 + 2*t^2.73 + 2*t^3.27 + t^3.82 + 3*t^4.36 + 3*t^4.91 + 3*t^5.45 + t^6. - t^4.09/y - t^4.09*y detail {a: 1455/2662, c: 3515/5324, X1: 18/11, M1: 10/11, M2: 4/11, M3: 12/11, q1: 9/11, q2: 9/11, qb1: 3/11, qb2: 7/11, phi1: 4/11}