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
46692 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_2\phi_1q_2^2$ + $ M_1^2$ + $ \phi_1q_2^3\tilde{q}_1$ + $ M_3\phi_1q_2^2$ 0.5986 0.7314 0.8184 [X:[], M:[1.0, 0.875, 0.875], q:[0.625, 0.375], qb:[0.5, 1.0], phi:[0.375]] [X:[], M:[[0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 9807/16384, c: 11983/16384, M1: 1, M2: 7/8, M3: 7/8, q1: 5/8, q2: 3/8, qb1: 1/2, qb2: 1, phi1: 3/8}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1^2$, $ M_2$, $ M_3$, $ q_2\tilde{q}_1$, $ M_1$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2\tilde{q}_2$, $ \phi_1^4$, $ \tilde{q}_1\tilde{q}_2$, $ M_2\phi_1^2$, $ M_3\phi_1^2$, $ \phi_1^2q_2\tilde{q}_1$, $ q_1\tilde{q}_2$, $ M_2^2$, $ M_2M_3$, $ M_3^2$, $ M_1\phi_1^2$, $ M_2q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_1M_2$, $ M_1M_3$, $ \phi_1\tilde{q}_1\tilde{q}_2$ $\phi_1^3q_2\tilde{q}_1$ -1 t^2.25 + 3*t^2.62 + t^3. + t^3.75 + 2*t^4.12 + 2*t^4.5 + 4*t^4.88 + 6*t^5.25 + t^5.62 - t^6. + 2*t^6.38 + 5*t^6.75 + 5*t^7.12 + 6*t^7.5 + 7*t^7.88 - 4*t^8.62 - t^4.12/y - t^6.38/y - (2*t^6.75)/y + (2*t^7.5)/y + (4*t^7.88)/y + (4*t^8.25)/y + (2*t^8.62)/y - t^4.12*y - t^6.38*y - 2*t^6.75*y + 2*t^7.5*y + 4*t^7.88*y + 4*t^8.25*y + 2*t^8.62*y t^2.25 + 3*t^2.62 + t^3. + t^3.75 + 2*t^4.12 + 2*t^4.5 + 4*t^4.88 + 6*t^5.25 + t^5.62 - t^6. + 2*t^6.38 + 5*t^6.75 + 5*t^7.12 + 6*t^7.5 + 7*t^7.88 - 4*t^8.62 - t^4.12/y - t^6.38/y - (2*t^6.75)/y + (2*t^7.5)/y + (4*t^7.88)/y + (4*t^8.25)/y + (2*t^8.62)/y - t^4.12*y - t^6.38*y - 2*t^6.75*y + 2*t^7.5*y + 4*t^7.88*y + 4*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
46986 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_2\phi_1q_2^2$ + $ M_1^2$ + $ \phi_1q_2^3\tilde{q}_1$ + $ M_3\phi_1q_2^2$ + $ M_4\phi_1^2$ 0.5795 0.6967 0.8318 [X:[], M:[1.0, 0.875, 0.875, 1.25], q:[0.625, 0.375], qb:[0.5, 1.0], phi:[0.375]] 3*t^2.62 + t^3. + 2*t^3.75 + 2*t^4.12 + t^4.5 + t^4.88 + 5*t^5.25 + t^5.62 - 2*t^6. - t^4.12/y - t^4.12*y detail {a: 9495/16384, c: 11415/16384, M1: 1, M2: 7/8, M3: 7/8, M4: 5/4, q1: 5/8, q2: 3/8, qb1: 1/2, qb2: 1, 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
46199 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_2\phi_1q_2^2$ + $ M_1^2$ + $ \phi_1q_2^3\tilde{q}_1$ 0.5874 0.7124 0.8245 [X:[], M:[1.0, 0.875], q:[0.625, 0.375], qb:[0.5, 1.0], phi:[0.375]] t^2.25 + 2*t^2.62 + t^3. + t^3.38 + t^3.75 + 2*t^4.12 + 2*t^4.5 + 3*t^4.88 + 3*t^5.25 + t^5.62 + t^6. - t^4.12/y - t^4.12*y detail {a: 1203/2048, c: 1459/2048, M1: 1, M2: 7/8, q1: 5/8, q2: 3/8, qb1: 1/2, qb2: 1, phi1: 3/8}