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
55165 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ + $ M_5\phi_1q_1^2$ + $ M_2M_5$ + $ M_4X_1$ + $ q_2\tilde{q}_1$ + $ \phi_1^2X_2$ 0.3537 0.4162 0.8498 [X:[1.5714, 1.4286], M:[0.8571, 0.7143, 1.1429, 0.4286, 1.2857], q:[0.2143, 0.9286], qb:[1.0714, 0.6429], phi:[0.2857]] [X:[[0], [0]], M:[[0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 1941/5488, c: 571/1372, X1: 11/7, X2: 10/7, M1: 6/7, M2: 5/7, M3: 8/7, M4: 3/7, M5: 9/7, q1: 3/14, q2: 13/14, qb1: 15/14, qb2: 9/14, phi1: 2/7}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_2$, $ M_1$, $ M_3$, $ \phi_1q_1\tilde{q}_2$, $ M_2^2$, $ \phi_1q_1q_2$, $ X_2$, $ M_1M_2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ X_1$, $ M_1^2$, $ \tilde{q}_1\tilde{q}_2$ . -1 t^2.14 + t^2.57 + t^3.43 + 2*t^4.29 + t^4.71 + t^5.14 - t^6. + t^6.43 + t^6.86 + t^7.71 - t^8.14 + t^8.57 - t^3.86/y + t^7.71/y + t^8.57/y - t^3.86*y + t^7.71*y + t^8.57*y t^2.14 + t^2.57 + t^3.43 + 2*t^4.29 + t^4.71 + t^5.14 - t^6. + t^6.43 + t^6.86 + t^7.71 - t^8.14 + t^8.57 - t^3.86/y + t^7.71/y + t^8.57/y - t^3.86*y + t^7.71*y + t^8.57*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
46915 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ + $ M_5\phi_1q_1^2$ + $ M_2M_5$ + $ M_4X_1$ 0.57 0.6947 0.8205 [X:[1.4014], M:[1.1972, 0.9977, 0.8028, 0.5986, 1.0023], q:[0.2993, 0.5035], qb:[0.703, 0.8979], phi:[0.3991]] t^2.39 + t^2.41 + t^2.99 + t^3.01 + t^3.59 + t^3.61 + t^3.62 + t^4.2 + t^4.22 + t^4.79 + 2*t^4.8 + t^4.82 + t^5.4 + t^5.42 + t^5.99 - t^4.2/y - t^4.2*y detail