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
46012 SU2adj1nf2 $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ q_1q_2\tilde{q}_1^2$ + $ q_1\tilde{q}_1\tilde{q}_2^2$ 0.6146 0.7604 0.8082 [X:[], M:[1.1667], q:[0.75, 0.4167], qb:[0.4167, 0.4167], phi:[0.5]] [X:[], M:[[0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 59/96, c: 73/96, M1: 7/6, q1: 3/4, q2: 5/12, qb1: 5/12, qb2: 5/12, phi1: 1/2}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$q_2\tilde{q}_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1^2$, $ M_1$, $ q_1q_2$, $ q_1\tilde{q}_1$, $ q_1\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_1^2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ \phi_1^2q_2\tilde{q}_1$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$ $q_1\tilde{q}_1^2\tilde{q}_2$ -1 2*t^2.5 + t^3. + 4*t^3.5 + 6*t^4. + 3*t^5. + 2*t^5.5 - t^6. + 10*t^6.5 + 7*t^7. + 12*t^7.5 + 15*t^8. - 6*t^8.5 - t^4.5/y + t^7./y + (2*t^8.5)/y - t^4.5*y + t^7.*y + 2*t^8.5*y 2*t^2.5 + t^3. + 4*t^3.5 + 6*t^4. + 3*t^5. + 2*t^5.5 - t^6. + 10*t^6.5 + 7*t^7. + 12*t^7.5 + 15*t^8. - 6*t^8.5 - t^4.5/y + t^7./y + (2*t^8.5)/y - t^4.5*y + t^7.*y + 2*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


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
45918 SU2adj1nf2 $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ q_1q_2\tilde{q}_1^2$ 0.6148 0.761 0.8079 [X:[], M:[1.1605], q:[0.75, 0.4289], qb:[0.4105, 0.4105], phi:[0.5]] t^2.46 + t^2.52 + t^3. + 3*t^3.48 + t^3.54 + 3*t^3.96 + 2*t^4.02 + t^4.07 + t^4.93 + t^4.98 + t^5.04 + t^5.46 + t^5.52 + t^5.94 - t^6. - t^4.5/y - t^4.5*y detail