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
447 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_1^2$ + $ \phi_1\tilde{q}_1^3\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_2M_3$ 0.57 0.695 0.8201 [X:[], M:[1.0, 0.8, 1.2], q:[0.6, 1.0], qb:[0.4, 0.4], phi:[0.4]] [X:[], M:[[0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 57/100, c: 139/200, M1: 1, M2: 4/5, M3: 6/5, q1: 3/5, q2: 1, qb1: 2/5, qb2: 2/5, phi1: 2/5}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_1$, $ q_1\tilde{q}_2$, $ M_3$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_2^2$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ \phi_1^4$, $ q_1q_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_1\phi_1^2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_1\tilde{q}_2^2$ $M_3\phi_1^2$, $ \phi_1^3\tilde{q}_1^2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ \phi_1^3\tilde{q}_2^2$, $ q_1^2\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2^3$ 4 2*t^2.4 + 2*t^3. + 3*t^3.6 + 2*t^4.2 + 4*t^4.8 + 2*t^5.4 + 4*t^6. + 4*t^6.6 + 7*t^7.2 + 4*t^7.8 + 4*t^8.4 - t^4.2/y - t^6.6/y + (2*t^7.8)/y + (4*t^8.4)/y - t^4.2*y - t^6.6*y + 2*t^7.8*y + 4*t^8.4*y 2*t^2.4 + 2*t^3. + 3*t^3.6 + 2*t^4.2 + 4*t^4.8 + 2*t^5.4 + 4*t^6. + 4*t^6.6 + 7*t^7.2 + 4*t^7.8 + 4*t^8.4 - t^4.2/y - t^6.6/y + (2*t^7.8)/y + (4*t^8.4)/y - t^4.2*y - t^6.6*y + 2*t^7.8*y + 4*t^8.4*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
747 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_1^2$ + $ \phi_1\tilde{q}_1^3\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_2M_3$ + $ M_4\tilde{q}_1\tilde{q}_2$ 0.5535 0.666 0.8311 [X:[], M:[1.0, 0.8, 1.2, 1.2], q:[0.6, 1.0], qb:[0.4, 0.4], phi:[0.4]] t^2.4 + 2*t^3. + 4*t^3.6 + 2*t^4.2 + 2*t^4.8 + 2*t^6. - t^4.2/y - t^4.2*y detail {a: 1107/2000, c: 333/500, M1: 1, M2: 4/5, M3: 6/5, M4: 6/5, q1: 3/5, q2: 1, qb1: 2/5, qb2: 2/5, phi1: 2/5}


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
278 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_1^2$ + $ \phi_1\tilde{q}_1^3\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ 0.5865 0.724 0.8101 [X:[], M:[1.0, 0.8], q:[0.6, 1.0], qb:[0.4, 0.4], phi:[0.4]] 3*t^2.4 + 2*t^3. + 2*t^3.6 + 2*t^4.2 + 7*t^4.8 + 4*t^5.4 + 4*t^6. - t^4.2/y - t^4.2*y detail {a: 1173/2000, c: 181/250, M1: 1, M2: 4/5, q1: 3/5, q2: 1, qb1: 2/5, qb2: 2/5, phi1: 2/5}