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
46411 SU2adj1nf2 $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_1M_3$ + $ q_2\tilde{q}_1\tilde{q}_2^2$ 0.5493 0.7074 0.7765 [X:[], M:[1.0588, 0.8235, 0.9412], q:[0.7647, 0.1765], qb:[0.5294, 0.6471], phi:[0.4706]] [X:[], M:[[0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 43179/78608, c: 27803/39304, M1: 18/17, M2: 14/17, M3: 16/17, q1: 13/17, q2: 3/17, qb1: 9/17, qb2: 11/17, phi1: 8/17}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$q_2\tilde{q}_1$, $ M_2$, $ \phi_1q_2^2$, $ q_2\tilde{q}_2$, $ M_3$, $ \phi_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_1q_2$, $ q_2^2\tilde{q}_1^2$, $ q_1\tilde{q}_2$, $ M_2q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_2^2$, $ M_2\phi_1q_2^2$, $ \phi_1^2q_2^4$, $ M_3q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_2q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_2M_3$, $ M_2\phi_1^2$, $ M_3\phi_1q_2^2$, $ \phi_1^3q_2^2$, $ \phi_1q_1\tilde{q}_1$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_3^2$, $ M_3\phi_1^2$, $ \phi_1^4$, $ \phi_1q_1\tilde{q}_2$ $M_2\tilde{q}_1\tilde{q}_2$ 0 t^2.12 + 3*t^2.47 + 2*t^2.82 + t^3.53 + 2*t^3.88 + 2*t^4.24 + 3*t^4.59 + 8*t^4.94 + 7*t^5.29 + t^5.65 + 5*t^6.35 + 6*t^6.71 + 5*t^7.06 + 12*t^7.41 + 14*t^7.76 + 4*t^8.12 - 5*t^8.47 + 2*t^8.82 - t^4.41/y - t^6.88/y - t^7.24/y + (4*t^7.59)/y + (6*t^7.94)/y + (6*t^8.29)/y + (2*t^8.65)/y - t^4.41*y - t^6.88*y - t^7.24*y + 4*t^7.59*y + 6*t^7.94*y + 6*t^8.29*y + 2*t^8.65*y t^2.12 + 3*t^2.47 + 2*t^2.82 + t^3.53 + 2*t^3.88 + 2*t^4.24 + 3*t^4.59 + 8*t^4.94 + 7*t^5.29 + t^5.65 + 5*t^6.35 + 6*t^6.71 + 5*t^7.06 + 12*t^7.41 + 14*t^7.76 + 4*t^8.12 - 5*t^8.47 + 2*t^8.82 - t^4.41/y - t^6.88/y - t^7.24/y + (4*t^7.59)/y + (6*t^7.94)/y + (6*t^8.29)/y + (2*t^8.65)/y - t^4.41*y - t^6.88*y - t^7.24*y + 4*t^7.59*y + 6*t^7.94*y + 6*t^8.29*y + 2*t^8.65*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
46176 SU2adj1nf2 $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_1M_3$ 0.6123 0.7911 0.7741 [X:[], M:[0.9708, 0.7135, 1.0292], q:[0.7427, 0.2865], qb:[0.4854, 0.4269], phi:[0.5146]] 2*t^2.14 + t^2.32 + t^2.74 + 2*t^3.09 + t^3.26 + t^3.51 + 2*t^3.68 + t^4.11 + 4*t^4.28 + 3*t^4.46 + t^4.63 + 2*t^4.88 + t^5.05 + 4*t^5.23 + 3*t^5.4 + t^5.47 + 2*t^5.65 + 5*t^5.82 - t^6. - t^4.54/y - t^4.54*y detail