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.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 44971 | SO5adj1nf2 | $q_1^2$ + $ \phi_1^2X_1$ + $ \phi_1^8$ + $ q_2^2X_2$ | 1.1265 | 1.1421 | 0.9863 | [X:[1.5, 1.5], M:[], q:[1.0, 0.25], qb:[], phi:[0.25]] | [X:[[0], [0]], M:[], q:[[0], [0]], qb:[], phi:[[0]]] | 0 | {a: 2307/2048, c: 2339/2048, X1: 3/2, X2: 3/2, q1: 1, q2: 1/4, phi1: 1/4} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $\phi_1^2q_2$, $ \phi_1^4$, $ \phi_1^2q_2^2$, $ \phi_1^4q_2^2$, $ X_1$, $ X_2$, $ \phi_1^6q_2$, $ \phi_1^4q_2^3$ | $\phi_1^6q_2^2$, $ \phi_1^4q_2^4$ | 2 | t^2.25 + 2*t^3. + 3*t^4.5 + 2*t^5.25 + 2*t^6. + 2*t^6.75 + 5*t^7.5 + 3*t^8.25 + t^8.25/y^2 - t^3.75/y - t^4.5/y - t^5.25/y - t^6./y - (2*t^6.75)/y - (2*t^7.5)/y - t^8.25/y - t^3.75*y - t^4.5*y - t^5.25*y - t^6.*y - 2*t^6.75*y - 2*t^7.5*y - t^8.25*y + t^8.25*y^2 | t^2.25 + 2*t^3. + 3*t^4.5 + 2*t^5.25 + 2*t^6. + 2*t^6.75 + 5*t^7.5 + 3*t^8.25 + t^8.25/y^2 - t^3.75/y - t^4.5/y - t^5.25/y - t^6./y - (2*t^6.75)/y - (2*t^7.5)/y - t^8.25/y - t^3.75*y - t^4.5*y - t^5.25*y - t^6.*y - 2*t^6.75*y - 2*t^7.5*y - t^8.25*y + t^8.25*y^2 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 8279 | SO5adj1nf1 | $\phi_1^2X_1$ + $ \phi_1^8$ + $ q_1^2X_2$ | 1.1265 | 1.1421 | 0.9863 | [X:[1.5, 1.5], M:[], q:[0.25], qb:[], phi:[0.25]] | t^2.25 + 2*t^3. + 3*t^4.5 + 2*t^5.25 + 2*t^6. - t^3.75/y - t^4.5/y - t^5.25/y - t^6./y - t^3.75*y - t^4.5*y - t^5.25*y - t^6.*y | detail | {a: 2307/2048, c: 2339/2048, X1: 3/2, X2: 3/2, q1: 1/4, phi1: 1/4} |
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.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 44924 | SO5adj1nf2 | $q_1^2$ + $ \phi_1^2X_1$ | 1.1741 | 1.206 | 0.9736 | [X:[1.5686], M:[], q:[1.0, 0.3528], qb:[], phi:[0.2157]] | t^2.12 + t^2.35 + t^2.59 + t^3.41 + t^4.23 + t^4.47 + 3*t^4.71 + t^4.94 + t^5.18 + t^5.53 + t^5.76 - t^3.65/y - t^4.71/y - t^4.94/y - t^5.76/y - t^6./y - t^3.65*y - t^4.71*y - t^4.94*y - t^5.76*y - t^6.*y | detail |