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
2 SU2adj1nf1 $\phi_1^2X_1$ + $ M_1q_1\tilde{q}_1$ 0.4583 0.5 0.9167 [X:[1.5556], M:[0.8889], q:[0.5556], qb:[0.5556], phi:[0.2222]] [X:[[0, 2]], M:[[0, -4]], q:[[-1, 4]], qb:[[1, 0]], phi:[[0, -1]]] 2 {a: 11/24, c: 1/2, X1: 14/9, M1: 8/9, q1: 5/9, qb1: 5/9, phi1: 2/9}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1^2$, $ X_1$, $ M_1^2$ . -4 t^2.67 + 3*t^4. + t^4.67 + t^5.33 - 4*t^6. + t^7.33 + 7*t^8. - t^8.67 - t^3.67/y - t^6.33/y + t^7./y - t^3.67*y - t^6.33*y + t^7.*y t^2.67/g2^4 + (g1^2*t^4.)/g2 + g2^3*t^4. + (g2^7*t^4.)/g1^2 + g2^2*t^4.67 + t^5.33/g2^8 - 2*t^6. - (g1^2*t^6.)/g2^4 - (g2^4*t^6.)/g1^2 + t^7.33/g2^2 + t^8./g2^12 + t^8./g2^3 + (g1^4*t^8.)/g2^2 + g1^2*g2^2*t^8. + g2^6*t^8. + (g2^10*t^8.)/g1^2 + (g2^14*t^8.)/g1^4 - t^8.67/g2^4 - t^3.67/(g2*y) - t^6.33/(g2^5*y) + (g2^3*t^7.)/y - (t^3.67*y)/g2 - (t^6.33*y)/g2^5 + g2^3*t^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
6 $\phi_1^2X_1$ + $ M_1q_1\tilde{q}_1$ + $ M_1^2$ 0.4526 0.4995 0.9062 [X:[1.5], M:[1.0], q:[0.5], qb:[0.5], phi:[0.25]] t^3. + 3*t^3.75 + t^4.5 - 3*t^6. - t^3.75/y - t^3.75*y detail {a: 927/2048, c: 1023/2048, X1: 3/2, M1: 1, q1: 1/2, qb1: 1/2, phi1: 1/4}


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
67 SU2adj1nf2 $\phi_1q_1^2$ + $ q_1q_2$ + $ \phi_1^2X_1$ + $ M_1\tilde{q}_1\tilde{q}_2$ 0.4583 0.5 0.9167 [X:[1.5556], M:[0.8889], q:[0.8889, 1.1111], qb:[0.5556, 0.5556], phi:[0.2222]] t^2.67 + 3*t^4. + t^4.67 + t^5.33 - 4*t^6. - t^3.67/y - t^3.67*y detail {a: 11/24, c: 1/2, X1: 14/9, M1: 8/9, q1: 8/9, q2: 10/9, qb1: 5/9, qb2: 5/9, phi1: 2/9}


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
1 SU2adj1nf1 $\phi_1^2X_1$ 0.4527 0.4986 0.9078 [X:[1.5042], M:[], q:[0.5042], qb:[0.5042], phi:[0.2479]] t^3.03 + 3*t^3.77 + t^4.51 - 4*t^6. - t^3.74/y - t^3.74*y detail