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
3282 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ + $ M_4q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_2$ + $ q_2\tilde{q}_2$ + $ M_4X_2$ + $ \phi_1^2X_3$ + $ M_5^2$ 0.4274 0.4962 0.8614 [X:[1.6, 1.8, 1.4], M:[1.2, 0.4, 0.8, 0.2, 1.0], q:[0.35, 1.35], qb:[0.45, 0.65], phi:[0.3]] [X:[[0], [0], [0]], M:[[0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 13677/32000, c: 15877/32000, X1: 8/5, X2: 9/5, X3: 7/5, M1: 6/5, M2: 2/5, M3: 4/5, M4: 1/5, M5: 1, q1: 7/20, q2: 27/20, qb1: 9/20, qb2: 13/20, phi1: 3/10}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_3$, $ M_5$, $ \tilde{q}_1\tilde{q}_2$, $ M_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ X_3$, $ M_3^2$, $ X_1$, $ M_3M_5$, $ X_2$ . 0 t^2.4 + t^3. + t^3.3 + t^3.6 + t^4.2 + t^4.8 + t^5.4 + t^6.6 + t^7.2 + t^7.8 - t^3.9/y + t^8.4/y + t^8.7/y - t^3.9*y + t^8.4*y + t^8.7*y t^2.4 + t^3. + t^3.3 + t^3.6 + t^4.2 + t^4.8 + t^5.4 + t^6.6 + t^7.2 + t^7.8 - t^3.9/y + t^8.4/y + t^8.7/y - t^3.9*y + t^8.4*y + t^8.7*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
3720 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ + $ M_4q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_2$ + $ q_2\tilde{q}_2$ + $ M_4X_2$ + $ \phi_1^2X_3$ + $ M_5^2$ + $ M_1M_6$ 0.4439 0.5252 0.8453 [X:[1.6, 1.8, 1.4], M:[1.2, 0.4, 0.8, 0.2, 1.0, 0.8], q:[0.35, 1.35], qb:[0.45, 0.65], phi:[0.3]] 2*t^2.4 + t^3. + t^3.3 + t^4.2 + 3*t^4.8 + 2*t^5.4 + t^5.7 - t^6. - t^3.9/y - t^3.9*y detail {a: 2841/6400, c: 3361/6400, X1: 8/5, X2: 9/5, X3: 7/5, M1: 6/5, M2: 2/5, M3: 4/5, M4: 1/5, M5: 1, M6: 4/5, q1: 7/20, q2: 27/20, qb1: 9/20, qb2: 13/20, phi1: 3/10}


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
2769 SU2adj1nf2 $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ + $ M_4q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_2$ + $ q_2\tilde{q}_2$ + $ M_4X_2$ + $ \phi_1^2X_3$ 0.4644 0.5384 0.8625 [X:[1.826, 1.6305, 1.4565], M:[1.087, 0.174, 0.913, 0.3695, 0.7175], q:[0.5054, 1.2229], qb:[0.4076, 0.7771], phi:[0.2718]] t^2.15 + t^2.74 + t^3.26 + t^3.55 + t^4.31 + t^4.37 + t^4.89 + t^5.41 + t^5.48 - t^6. - t^3.82/y - t^5.97/y - t^3.82*y - t^5.97*y detail