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
56629 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_3M_4$ + $ \phi_1^2q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1\tilde{q}_1^2$ + $ M_2X_1$ + $ M_6\phi_1q_2\tilde{q}_2$ + $ M_1\phi_1^2$ 0.6443 0.8125 0.7929 [X:[1.3846], M:[1.0769, 0.6154, 0.7692, 1.2308, 0.7692, 0.7692], q:[0.6154, 0.3077], qb:[0.7692, 0.4615], phi:[0.4615]] [X:[[0]], M:[[0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 22647/35152, c: 14281/17576, X1: 18/13, M1: 14/13, M2: 8/13, M3: 10/13, M4: 16/13, M5: 10/13, M6: 10/13, q1: 8/13, q2: 4/13, qb1: 10/13, qb2: 6/13, phi1: 6/13}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_3$, $ M_5$, $ M_6$, $ \phi_1^2$, $ M_1$, $ \phi_1q_2^2$, $ q_2\tilde{q}_1$, $ q_1\tilde{q}_2$, $ \phi_1q_1q_2$, $ \phi_1\tilde{q}_2^2$, $ X_1$, $ M_3^2$, $ M_3M_5$, $ M_5^2$, $ M_3M_6$, $ M_5M_6$, $ M_6^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_3\phi_1^2$, $ M_5\phi_1^2$, $ M_6\phi_1^2$, $ \phi_1q_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1M_3$, $ M_1M_5$, $ M_1M_6$, $ \phi_1^4$, $ M_3\phi_1q_2^2$, $ M_5\phi_1q_2^2$, $ M_6\phi_1q_2^2$, $ \phi_1q_1\tilde{q}_1$, $ M_5q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ M_3q_1\tilde{q}_2$, $ M_5q_1\tilde{q}_2$, $ M_6q_1\tilde{q}_2$ $\phi_1^3q_2^2$, $ \phi_1^2q_1\tilde{q}_2$ 0 3*t^2.31 + t^2.77 + 4*t^3.23 + 3*t^4.15 + 7*t^4.62 + 3*t^5.08 + 11*t^5.54 + 11*t^6.46 + 8*t^6.92 + 10*t^7.38 + 18*t^7.85 - t^8.31 + 19*t^8.77 - t^4.38/y - (2*t^6.69)/y + (3*t^7.62)/y + (5*t^8.08)/y + (12*t^8.54)/y - t^4.38*y - 2*t^6.69*y + 3*t^7.62*y + 5*t^8.08*y + 12*t^8.54*y 3*t^2.31 + t^2.77 + 4*t^3.23 + 3*t^4.15 + 7*t^4.62 + 3*t^5.08 + 11*t^5.54 + 11*t^6.46 + 8*t^6.92 + 10*t^7.38 + 18*t^7.85 - t^8.31 + 19*t^8.77 - t^4.38/y - (2*t^6.69)/y + (3*t^7.62)/y + (5*t^8.08)/y + (12*t^8.54)/y - t^4.38*y - 2*t^6.69*y + 3*t^7.62*y + 5*t^8.08*y + 12*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
55036 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_3M_4$ + $ \phi_1^2q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1\tilde{q}_1^2$ + $ M_2X_1$ + $ M_6\phi_1q_2\tilde{q}_2$ 0.6554 0.8206 0.7987 [X:[1.4999], M:[0.9287, 0.5001, 0.7857, 1.2143, 0.7857, 0.7857], q:[0.7142, 0.3571], qb:[0.7857, 0.4286], phi:[0.4286]] 3*t^2.36 + t^2.57 + t^2.79 + 3*t^3.43 + t^3.86 + 2*t^4.5 + 7*t^4.71 + 2*t^4.93 + 3*t^5.14 + t^5.36 + 2*t^5.57 + 8*t^5.79 - t^6. - t^4.29/y - t^4.29*y detail