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
431 SU2adj1nf2 $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_1M_3$ + $ M_2^2$ + $ M_1\phi_1^2$ 0.6363 0.7702 0.8261 [X:[], M:[1.1429, 1.0, 0.8571], q:[0.7857, 0.3571], qb:[0.5, 0.6429], phi:[0.4286]] [X:[], M:[[0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 873/1372, c: 4227/5488, M1: 8/7, M2: 1, M3: 6/7, q1: 11/14, q2: 5/14, qb1: 1/2, qb2: 9/14, phi1: 3/7}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_3$, $ \phi_1^2$, $ M_2$, $ M_1$, $ q_1q_2$, $ \phi_1q_2^2$, $ q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ M_3\phi_1^2$, $ \phi_1^4$, $ \phi_1\tilde{q}_2^2$ $M_3q_1q_2$, $ M_3\phi_1q_2^2$, $ \phi_1^3q_2^2$ 3 2*t^2.57 + t^3. + 3*t^3.43 + 2*t^3.86 + 3*t^4.29 + t^4.71 + 3*t^5.14 + 3*t^6. + 2*t^6.43 + 6*t^6.86 + 5*t^7.29 + 9*t^7.71 + 3*t^8.14 + 4*t^8.57 - t^4.29/y - t^6.86/y + t^7.71/y + t^8.14/y + (2*t^8.57)/y - t^4.29*y - t^6.86*y + t^7.71*y + t^8.14*y + 2*t^8.57*y 2*t^2.57 + t^3. + 3*t^3.43 + 2*t^3.86 + 3*t^4.29 + t^4.71 + 3*t^5.14 + 3*t^6. + 2*t^6.43 + 6*t^6.86 + 5*t^7.29 + 9*t^7.71 + 3*t^8.14 + 4*t^8.57 - t^4.29/y - t^6.86/y + t^7.71/y + t^8.14/y + (2*t^8.57)/y - t^4.29*y - t^6.86*y + t^7.71*y + t^8.14*y + 2*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
268 SU2adj1nf2 $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_1M_3$ + $ M_2^2$ 0.6707 0.8047 0.8336 [X:[], M:[1.0, 1.0, 1.0], q:[0.7857, 0.5], qb:[0.5, 0.5], phi:[0.4286]] t^2.57 + 3*t^3. + 3*t^3.86 + 6*t^4.29 + t^5.14 + 3*t^5.57 - 3*t^6. - t^4.29/y - t^4.29*y detail {a: 3681/5488, c: 276/343, M1: 1, M2: 1, M3: 1, q1: 11/14, q2: 1/2, qb1: 1/2, qb2: 1/2, phi1: 3/7}