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
377 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_2\phi_1^2$ + $ q_2^2\tilde{q}_1^2$ + $ q_2^2\tilde{q}_2^2$ + $ M_1X_1$ 0.6489 0.7809 0.831 [X:[1.3333], M:[0.6667, 1.1111], q:[0.7778, 0.5556], qb:[0.4444, 0.4444], phi:[0.4444]] [X:[[0]], M:[[0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] 0 {a: 841/1296, c: 253/324, X1: 4/3, M1: 2/3, M2: 10/9, q1: 7/9, q2: 5/9, qb1: 4/9, qb2: 4/9, phi1: 4/9}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1^2$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ M_2$, $ q_1\tilde{q}_1$, $ q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ X_1$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1^4$, $ \phi_1q_1q_2$ $q_2^2\tilde{q}_1\tilde{q}_2$ -1 t^2.67 + 2*t^3. + t^3.33 + 2*t^3.67 + 4*t^4. + 2*t^4.33 + t^4.67 + t^5.33 - t^6. + 6*t^6.67 + 6*t^7. + 4*t^7.33 + 6*t^7.67 + 10*t^8. + 4*t^8.33 - t^8.67 - t^4.33/y + (2*t^8.67)/y - t^4.33*y + 2*t^8.67*y t^2.67 + 2*t^3. + t^3.33 + 2*t^3.67 + 4*t^4. + 2*t^4.33 + t^4.67 + t^5.33 - t^6. + 6*t^6.67 + 6*t^7. + 4*t^7.33 + 6*t^7.67 + 10*t^8. + 4*t^8.33 - t^8.67 - t^4.33/y + (2*t^8.67)/y - t^4.33*y + 2*t^8.67*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
220 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_2\phi_1^2$ + $ q_2^2\tilde{q}_1^2$ 0.6709 0.8239 0.8143 [X:[], M:[0.6905, 1.1032], q:[0.7758, 0.5338], qb:[0.4662, 0.4306], phi:[0.4484]] t^2.07 + t^2.69 + t^2.89 + t^3. + t^3.31 + t^3.62 + t^3.73 + t^3.93 + t^4.04 + 2*t^4.14 + t^4.24 + t^4.35 + t^4.55 + t^4.76 + t^4.96 + t^5.07 + 2*t^5.38 + t^5.58 + t^5.69 + t^5.79 - t^4.35/y - t^4.35*y detail