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
773 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_1^2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_2X_1$ + $ \phi_1^2X_2$ + $ M_1M_4$ + $ M_3^2$ 0.5176 0.6192 0.836 [X:[1.625, 1.25], M:[0.875, 0.375, 1.0, 1.125], q:[0.875, 0.75], qb:[0.25, 0.625], phi:[0.375]] [X:[[0], [0]], M:[[0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 8481/16384, c: 10145/16384, X1: 13/8, X2: 5/4, M1: 7/8, M2: 3/8, M3: 1, M4: 9/8, q1: 7/8, q2: 3/4, qb1: 1/4, qb2: 5/8, phi1: 3/8}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ \tilde{q}_1\tilde{q}_2$, $ M_3$, $ M_4$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ X_2$, $ q_2\tilde{q}_2$, $ q_1\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_1M_3$, $ M_3\tilde{q}_1\tilde{q}_2$ . -1 2*t^2.62 + t^3. + t^3.38 + 2*t^3.75 + t^4.12 + t^4.5 + t^4.88 + 2*t^5.25 + t^5.62 - t^6. + 2*t^6.38 + 2*t^6.75 + t^7.12 + 2*t^7.5 + 3*t^7.88 + 3*t^8.25 - 2*t^8.62 - t^4.12/y + t^8.25/y + (2*t^8.62)/y - t^4.12*y + t^8.25*y + 2*t^8.62*y 2*t^2.62 + t^3. + t^3.38 + 2*t^3.75 + t^4.12 + t^4.5 + t^4.88 + 2*t^5.25 + t^5.62 - t^6. + 2*t^6.38 + 2*t^6.75 + t^7.12 + 2*t^7.5 + 3*t^7.88 + 3*t^8.25 - 2*t^8.62 - t^4.12/y + t^8.25/y + (2*t^8.62)/y - t^4.12*y + t^8.25*y + 2*t^8.62*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
1261 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_1^2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_2X_1$ + $ \phi_1^2X_2$ + $ M_1M_4$ + $ M_3^2$ + $ M_4M_5$ 0.5288 0.6382 0.8286 [X:[1.625, 1.25], M:[0.875, 0.375, 1.0, 1.125, 0.875], q:[0.875, 0.75], qb:[0.25, 0.625], phi:[0.375]] 3*t^2.62 + t^3. + 2*t^3.75 + t^4.12 + t^4.5 + t^4.88 + 5*t^5.25 + 2*t^5.62 - 3*t^6. - t^4.12/y - t^4.12*y detail {a: 1083/2048, c: 1307/2048, X1: 13/8, X2: 5/4, M1: 7/8, M2: 3/8, M3: 1, M4: 9/8, M5: 7/8, q1: 7/8, q2: 3/4, qb1: 1/4, qb2: 5/8, phi1: 3/8}


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
485 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_1^2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_2X_1$ + $ \phi_1^2X_2$ + $ M_1M_4$ 0.5465 0.65 0.8409 [X:[1.655, 1.31], M:[0.965, 0.345, 0.76, 1.035], q:[0.725, 0.93], qb:[0.31, 0.655], phi:[0.345]] t^2.28 + 2*t^2.9 + t^3.1 + 2*t^3.93 + t^4.14 + t^4.56 + t^4.76 + t^4.97 + t^5.17 + t^5.38 + 2*t^5.79 - 2*t^6. - t^4.03/y - t^4.03*y detail