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
275 SU2adj1nf2 $\phi_1q_1^2$ + $ q_1q_2$ + $ \phi_1^2X_1$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_1M_2$ + $ \tilde{q}_1^2\tilde{q}_2^2$ 0.3472 0.394 0.881 [X:[1.5], M:[0.75, 1.25], q:[0.875, 1.125], qb:[0.25, 0.75], phi:[0.25]] [X:[[0]], M:[[0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 711/2048, c: 807/2048, X1: 3/2, M1: 3/4, M2: 5/4, q1: 7/8, q2: 9/8, qb1: 1/4, qb2: 3/4, phi1: 1/4}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ \tilde{q}_1\tilde{q}_2$, $ M_2$, $ M_1^2$, $ X_1$, $ M_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$ . 0 t^2.25 + t^3. + t^3.75 + t^4.5 + t^5.25 + t^7.5 - t^3.75/y + t^8.25/y - t^3.75*y + t^8.25*y t^2.25 + t^3. + t^3.75 + t^4.5 + t^5.25 + t^7.5 - t^3.75/y + t^8.25/y - t^3.75*y + t^8.25*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
448 $\phi_1q_1^2$ + $ q_1q_2$ + $ \phi_1^2X_1$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_1M_2$ + $ \tilde{q}_1^2\tilde{q}_2^2$ + $ M_2M_3$ 0.3662 0.4287 0.8542 [X:[1.5], M:[0.75, 1.25, 0.75], q:[0.875, 1.125], qb:[0.25, 0.75], phi:[0.25]] 2*t^2.25 + t^3. + 3*t^4.5 + 2*t^5.25 - t^6. - t^3.75/y - t^6./y - t^3.75*y - t^6.*y detail {a: 375/1024, c: 439/1024, X1: 3/2, M1: 3/4, M2: 5/4, M3: 3/4, q1: 7/8, q2: 9/8, qb1: 1/4, qb2: 3/4, phi1: 1/4}


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
27 SU2adj1nf1 $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1q_1\tilde{q}_1$ + $ M_1M_2$ + $ q_1^2\tilde{q}_1^2$ 0.3472 0.394 0.881 [X:[1.5], M:[1.25, 0.75], q:[0.25], qb:[0.75], phi:[0.25]] t^2.25 + t^3. + t^3.75 + t^4.5 + t^5.25 - t^3.75/y - t^3.75*y detail {a: 711/2048, c: 807/2048, X1: 3/2, M1: 5/4, M2: 3/4, q1: 1/4, qb1: 3/4, phi1: 1/4}


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
176 SU2adj1nf2 $\phi_1q_1^2$ + $ q_1q_2$ + $ \phi_1^2X_1$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_1M_2$ 0.4135 0.4854 0.8518 [X:[1.3853], M:[0.922, 1.078], q:[0.8463, 1.1537], qb:[0.3073, 0.4634], phi:[0.3073]] t^2.31 + t^2.77 + t^3.23 + t^3.7 + t^4.16 + t^4.62 + t^5.08 + t^5.55 - t^6. - t^3.92/y - t^3.92*y detail