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
260 SU2adj1nf2 $\phi_1^4$ + $ M_1q_1q_2$ + $ q_1\tilde{q}_1^2\tilde{q}_2$ + $ \phi_1\tilde{q}_2^2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_1\tilde{q}_1$ 0.6003 0.7357 0.8159 [X:[], M:[1.1667, 1.1667], q:[0.4167, 0.4167], qb:[0.4167, 0.75], phi:[0.5]] [X:[], M:[[0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 461/768, c: 565/768, M1: 7/6, M2: 7/6, q1: 5/12, q2: 5/12, qb1: 5/12, qb2: 3/4, phi1: 1/2}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$q_2\tilde{q}_1$, $ \phi_1^2$, $ M_1$, $ M_2$, $ q_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_1^2$, $ \phi_1q_1q_2$, $ \phi_1q_2^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_1$ $M_2q_2\tilde{q}_1$, $ q_2\tilde{q}_1^2\tilde{q}_2$ -4 t^2.5 + t^3. + 5*t^3.5 + 6*t^4. + t^5. + t^5.5 - 4*t^6. + 5*t^6.5 + 12*t^7. + 15*t^7.5 + 13*t^8. - 4*t^8.5 - t^4.5/y + (2*t^7.)/y - (2*t^8.)/y + t^8.5/y - t^4.5*y + 2*t^7.*y - 2*t^8.*y + t^8.5*y t^2.5 + t^3. + 5*t^3.5 + 6*t^4. + t^5. + t^5.5 - 4*t^6. + 5*t^6.5 + 12*t^7. + 15*t^7.5 + 13*t^8. - 4*t^8.5 - t^4.5/y + (2*t^7.)/y - (2*t^8.)/y + t^8.5/y - t^4.5*y + 2*t^7.*y - 2*t^8.*y + t^8.5*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
409 $\phi_1^4$ + $ M_1q_1q_2$ + $ q_1\tilde{q}_1^2\tilde{q}_2$ + $ \phi_1\tilde{q}_2^2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ 0.5859 0.7109 0.8242 [X:[], M:[1.1667, 1.1667, 1.1667], q:[0.4167, 0.4167], qb:[0.4167, 0.75], phi:[0.5]] t^3. + 6*t^3.5 + 6*t^4. - 9*t^6. - t^4.5/y - t^4.5*y detail {a: 75/128, c: 91/128, M1: 7/6, M2: 7/6, M3: 7/6, q1: 5/12, q2: 5/12, qb1: 5/12, qb2: 3/4, phi1: 1/2}


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
167 SU2adj1nf2 $\phi_1^4$ + $ M_1q_1q_2$ + $ q_1\tilde{q}_1^2\tilde{q}_2$ + $ \phi_1\tilde{q}_2^2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ 0.6146 0.7604 0.8082 [X:[], M:[1.1667], q:[0.4167, 0.4167], qb:[0.4167, 0.75], phi:[0.5]] 2*t^2.5 + t^3. + 4*t^3.5 + 6*t^4. + 3*t^5. + 2*t^5.5 - t^6. - t^4.5/y - t^4.5*y detail {a: 59/96, c: 73/96, M1: 7/6, q1: 5/12, q2: 5/12, qb1: 5/12, qb2: 3/4, phi1: 1/2}