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
46664 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ q_2\tilde{q}_1\tilde{q}_2^2$ + $ \phi_1q_2^2\tilde{q}_1^2$ + $ M_2X_1$ 0.5167 0.6609 0.7818 [X:[1.3846], M:[1.0769, 0.6154, 0.9231], q:[0.7692, 0.1538], qb:[0.6154, 0.6154], phi:[0.4615]] [X:[[0]], M:[[0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 9081/17576, c: 1452/2197, X1: 18/13, M1: 14/13, M2: 8/13, M3: 12/13, q1: 10/13, q2: 2/13, qb1: 8/13, qb2: 8/13, phi1: 6/13}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1q_2^2$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ M_3$, $ \phi_1^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_1q_2$, $ q_1\tilde{q}_2$, $ X_1$, $ \phi_1^2q_2^4$, $ \phi_1q_2^3\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ \phi_1q_2^3\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_3\phi_1q_2^2$, $ \phi_1^3q_2^2$, $ M_3q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\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}_1$, $ \phi_1q_1\tilde{q}_2$ $\phi_1^2q_2^3\tilde{q}_1$, $ \phi_1^2q_2^3\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_2^2$ 1 3*t^2.31 + 2*t^2.77 + 3*t^3.69 + 2*t^4.15 + 4*t^4.62 + 9*t^5.08 + t^5.54 + t^6. + 7*t^6.46 + 4*t^6.92 + 11*t^7.38 + 10*t^7.85 - 5*t^8.31 + 5*t^8.77 - t^4.38/y - t^7.15/y + (4*t^7.62)/y + (6*t^8.08)/y + t^8.54/y - t^4.38*y - t^7.15*y + 4*t^7.62*y + 6*t^8.08*y + t^8.54*y 3*t^2.31 + 2*t^2.77 + 3*t^3.69 + 2*t^4.15 + 4*t^4.62 + 9*t^5.08 + t^5.54 + t^6. + 7*t^6.46 + 4*t^6.92 + 11*t^7.38 + 10*t^7.85 - 5*t^8.31 + 5*t^8.77 - t^4.38/y - t^7.15/y + (4*t^7.62)/y + (6*t^8.08)/y + t^8.54/y - t^4.38*y - t^7.15*y + 4*t^7.62*y + 6*t^8.08*y + t^8.54*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
46203 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ q_2\tilde{q}_1\tilde{q}_2^2$ 0.5568 0.7209 0.7723 [X:[], M:[1.0504, 0.7481, 0.9496], q:[0.7626, 0.187], qb:[0.4893, 0.6618], phi:[0.4748]] t^2.03 + t^2.24 + 2*t^2.55 + 2*t^2.85 + 2*t^3.45 + t^3.97 + t^4.06 + 2*t^4.27 + t^4.36 + t^4.49 + t^4.58 + 2*t^4.79 + 3*t^4.88 + 4*t^5.09 + 5*t^5.4 + t^5.48 + 3*t^5.7 - t^4.42/y - t^4.42*y detail