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
55096 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_1M_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ q_2\tilde{q}_2$ + $ \phi_1^2X_1$ + $ M_4q_2\tilde{q}_1$ + $ M_3M_4$ + $ M_3M_5$ 0.4206 0.4975 0.8454 [X:[1.3846], M:[0.7692, 1.2308, 1.0769, 0.9231, 0.9231], q:[0.4615, 0.7692], qb:[0.3077, 1.2308], phi:[0.3077]] [X:[[0]], M:[[0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 924/2197, c: 1093/2197, X1: 18/13, M1: 10/13, M2: 16/13, M3: 14/13, M4: 12/13, M5: 12/13, q1: 6/13, q2: 10/13, qb1: 4/13, qb2: 16/13, phi1: 4/13}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ M_4$, $ M_5$, $ M_2$, $ \phi_1q_2\tilde{q}_1$, $ X_1$, $ M_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_1M_4$, $ M_1M_5$, $ q_1\tilde{q}_2$, $ M_4^2$, $ M_4M_5$, $ M_5^2$, $ \phi_1q_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$ . -1 t^2.31 + 2*t^2.77 + t^3.69 + t^4.15 + t^4.62 + 2*t^5.08 + 2*t^5.54 - t^6. + t^6.92 + t^7.38 + 2*t^7.85 + t^8.31 - 2*t^8.77 - t^3.92/y - t^6.69/y + t^7.15/y + (2*t^8.08)/y + t^8.54/y - t^3.92*y - t^6.69*y + t^7.15*y + 2*t^8.08*y + t^8.54*y t^2.31 + 2*t^2.77 + t^3.69 + t^4.15 + t^4.62 + 2*t^5.08 + 2*t^5.54 - t^6. + t^6.92 + t^7.38 + 2*t^7.85 + t^8.31 - 2*t^8.77 - t^3.92/y - t^6.69/y + t^7.15/y + (2*t^8.08)/y + t^8.54/y - t^3.92*y - t^6.69*y + t^7.15*y + 2*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
56760 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_1M_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ q_2\tilde{q}_2$ + $ \phi_1^2X_1$ + $ M_4q_2\tilde{q}_1$ + $ M_3M_4$ + $ M_3M_5$ + $ M_2M_6$ 0.4388 0.5301 0.8277 [X:[1.3846], M:[0.7692, 1.2308, 1.0769, 0.9231, 0.9231, 0.7692], q:[0.4615, 0.7692], qb:[0.3077, 1.2308], phi:[0.3077]] 2*t^2.31 + 2*t^2.77 + t^4.15 + 3*t^4.62 + 4*t^5.08 + 2*t^5.54 - 2*t^6. - t^3.92/y - t^3.92*y detail {a: 15423/35152, c: 9317/17576, X1: 18/13, M1: 10/13, M2: 16/13, M3: 14/13, M4: 12/13, M5: 12/13, M6: 10/13, q1: 6/13, q2: 10/13, qb1: 4/13, qb2: 16/13, phi1: 4/13}


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
46944 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_1M_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ q_2\tilde{q}_2$ + $ \phi_1^2X_1$ + $ M_4q_2\tilde{q}_1$ + $ M_3M_4$ 0.4135 0.4856 0.8515 [X:[1.3846], M:[0.7692, 1.2308, 1.0769, 0.9231], q:[0.4615, 0.7692], qb:[0.3077, 1.2308], phi:[0.3077]] t^2.31 + t^2.77 + t^3.23 + t^3.69 + t^4.15 + t^4.62 + t^5.08 + t^5.54 - t^3.92/y - t^3.92*y detail {a: 14535/35152, c: 8535/17576, X1: 18/13, M1: 10/13, M2: 16/13, M3: 14/13, M4: 12/13, q1: 6/13, q2: 10/13, qb1: 4/13, qb2: 16/13, phi1: 4/13}