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
56265 SU2adj1nf2 $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_2\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_2M_3$ + $ \phi_1q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ + $ M_6q_1\tilde{q}_2$ + $ M_6^2$ 0.6002 0.7609 0.7888 [X:[], M:[0.8571, 0.7143, 1.2857, 0.8571, 0.8571, 1.0], q:[0.7143, 0.4286], qb:[0.8571, 0.2857], phi:[0.4286]] [X:[], M:[[0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 1647/2744, c: 261/343, M1: 6/7, M2: 5/7, M3: 9/7, M4: 6/7, M5: 6/7, M6: 1, q1: 5/7, q2: 3/7, qb1: 6/7, qb2: 2/7, phi1: 3/7}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_2$, $ M_1$, $ M_4$, $ M_5$, $ \phi_1^2$, $ M_6$, $ \phi_1\tilde{q}_2^2$, $ M_3$, $ \phi_1q_2^2$, $ M_2^2$, $ \phi_1q_1\tilde{q}_2$, $ M_1M_2$, $ M_2M_4$, $ M_2M_5$, $ M_2\phi_1^2$, $ \phi_1q_1q_2$, $ q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ M_1M_4$, $ M_4^2$, $ M_1M_5$, $ M_4M_5$, $ M_5^2$, $ M_2M_6$, $ M_1\phi_1^2$, $ M_4\phi_1^2$, $ M_5\phi_1^2$, $ \phi_1^4$, $ \phi_1q_2\tilde{q}_1$, $ M_2\phi_1\tilde{q}_2^2$, $ M_1M_6$, $ M_4M_6$, $ M_5M_6$, $ M_6\phi_1^2$, $ \phi_1q_1^2$, $ M_1\phi_1\tilde{q}_2^2$, $ M_4\phi_1\tilde{q}_2^2$, $ M_5\phi_1\tilde{q}_2^2$ $M_2\phi_1q_2^2$, $ M_6\phi_1\tilde{q}_2^2$, $ \phi_1^2\tilde{q}_2^4$ 0 t^2.14 + 4*t^2.57 + 2*t^3. + 2*t^3.86 + t^4.29 + 5*t^4.71 + 12*t^5.14 + 6*t^5.57 + 5*t^6.43 + 2*t^6.86 + 10*t^7.29 + 27*t^7.71 + 8*t^8.14 - 6*t^8.57 - t^4.29/y - (4*t^6.86)/y + (8*t^7.71)/y + (8*t^8.14)/y + (8*t^8.57)/y - t^4.29*y - 4*t^6.86*y + 8*t^7.71*y + 8*t^8.14*y + 8*t^8.57*y t^2.14 + 4*t^2.57 + 2*t^3. + 2*t^3.86 + t^4.29 + 5*t^4.71 + 12*t^5.14 + 6*t^5.57 + 5*t^6.43 + 2*t^6.86 + 10*t^7.29 + 27*t^7.71 + 8*t^8.14 - 6*t^8.57 - t^4.29/y - (4*t^6.86)/y + (8*t^7.71)/y + (8*t^8.14)/y + (8*t^8.57)/y - t^4.29*y - 4*t^6.86*y + 8*t^7.71*y + 8*t^8.14*y + 8*t^8.57*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
50964 SU2adj1nf2 $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_2\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_2M_3$ + $ \phi_1q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ + $ M_6q_1\tilde{q}_2$ 0.6751 0.8593 0.7856 [X:[], M:[0.7632, 0.8553, 1.1447, 0.7632, 0.7632, 0.671], q:[0.8553, 0.3816], qb:[0.7632, 0.4737], phi:[0.3816]] t^2.01 + 4*t^2.29 + t^2.57 + 2*t^3.43 + t^3.99 + t^4.03 + 4*t^4.3 + 11*t^4.58 + 5*t^4.86 + t^5.13 + 2*t^5.45 + 6*t^5.72 - 2*t^6. - t^4.14/y - t^4.14*y detail