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
47069 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_1M_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ q_2\tilde{q}_2$ + $ \phi_1^2X_1$ + $ M_4q_2\tilde{q}_1$ + $ M_3^2$ 0.4365 0.5115 0.8534 [X:[1.4], M:[0.8, 1.2, 1.0, 0.9], q:[0.45, 0.75], qb:[0.35, 1.25], phi:[0.3]] [X:[[0]], M:[[0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 873/2000, c: 1023/2000, X1: 7/5, M1: 4/5, M2: 6/5, M3: 1, M4: 9/10, q1: 9/20, q2: 3/4, qb1: 7/20, qb2: 5/4, phi1: 3/10}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ M_4$, $ M_3$, $ M_2$, $ \phi_1q_2\tilde{q}_1$, $ X_1$, $ M_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_1M_4$, $ q_1\tilde{q}_2$, $ M_1M_3$, $ M_4^2$, $ \phi_1q_2^2$ . 0 t^2.4 + t^2.7 + t^3. + t^3.6 + t^4.2 + t^4.8 + t^5.1 + 2*t^5.4 + t^7.2 + 2*t^7.8 + t^8.1 - t^8.7 - t^3.9/y - t^6.6/y + t^7.2/y + t^8.1/y + t^8.4/y + t^8.7/y - t^3.9*y - t^6.6*y + t^7.2*y + t^8.1*y + t^8.4*y + t^8.7*y t^2.4 + t^2.7 + t^3. + t^3.6 + t^4.2 + t^4.8 + t^5.1 + 2*t^5.4 + t^7.2 + 2*t^7.8 + t^8.1 - t^8.7 - t^3.9/y - t^6.6/y + t^7.2/y + t^8.1/y + t^8.4/y + t^8.7/y - t^3.9*y - t^6.6*y + t^7.2*y + t^8.1*y + t^8.4*y + t^8.7*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
55119 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_1M_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ q_2\tilde{q}_2$ + $ \phi_1^2X_1$ + $ M_4q_2\tilde{q}_1$ + $ M_3^2$ + $ M_2M_5$ 0.453 0.5405 0.8381 [X:[1.4], M:[0.8, 1.2, 1.0, 0.9, 0.8], q:[0.45, 0.75], qb:[0.35, 1.25], phi:[0.3]] 2*t^2.4 + t^2.7 + t^3. + t^4.2 + 3*t^4.8 + 2*t^5.1 + 3*t^5.4 - t^6. - t^3.9/y - t^3.9*y detail {a: 453/1000, c: 1081/2000, X1: 7/5, M1: 4/5, M2: 6/5, M3: 1, M4: 9/10, M5: 4/5, q1: 9/20, q2: 3/4, qb1: 7/20, qb2: 5/4, phi1: 3/10}


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
46584 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_1M_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ q_2\tilde{q}_2$ + $ \phi_1^2X_1$ + $ M_4q_2\tilde{q}_1$ 0.4801 0.5664 0.8477 [X:[1.4601], M:[0.9203, 1.0797, 0.6994, 0.8098], q:[0.4049, 0.6748], qb:[0.5154, 1.3252], phi:[0.2699]] t^2.1 + t^2.43 + t^2.76 + t^3.24 + t^4.2 + t^4.38 + t^4.53 + 2*t^4.86 + t^5.19 + t^5.34 + t^5.52 - t^6. - t^3.81/y - t^5.91/y - t^3.81*y - t^5.91*y detail