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 |
|---|---|---|---|---|---|---|---|---|---|
| 1118 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_2M_4$ + $ M_1M_4$ + $ M_1M_5$ + $ M_3M_4$ | 0.6509 | 0.7903 | 0.8236 | [X:[], M:[1.0769, 1.0769, 1.0769, 0.9231, 0.9231], q:[0.7692, 0.4615], qb:[0.4615, 0.4615], phi:[0.4615]] | [X:[], M:[[0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 22881/35152, c: 13891/17576, M1: 14/13, M2: 14/13, M3: 14/13, M4: 12/13, M5: 12/13, q1: 10/13, q2: 6/13, qb1: 6/13, qb2: 6/13, phi1: 6/13} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_5$, $ \phi_1^2$, $ M_3$, $ q_1q_2$, $ q_1\tilde{q}_1$, $ q_1\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_4^2$, $ M_4M_5$, $ M_5^2$, $ M_4\phi_1^2$, $ M_5\phi_1^2$, $ \phi_1^4$ | $M_3M_5$, $ M_3\phi_1^2$ | -6 | 3*t^2.77 + t^3.23 + 3*t^3.69 + 6*t^4.15 + 6*t^5.54 - 6*t^6. + 6*t^6.46 + 15*t^6.92 - 2*t^7.38 + 10*t^7.85 + 22*t^8.31 - 21*t^8.77 - t^4.38/y + (3*t^8.54)/y - t^4.38*y + 3*t^8.54*y | 3*t^2.77 + t^3.23 + 3*t^3.69 + 6*t^4.15 + 6*t^5.54 - 6*t^6. + 6*t^6.46 + 15*t^6.92 - 2*t^7.38 + 10*t^7.85 + 22*t^8.31 - 21*t^8.77 - t^4.38/y + (3*t^8.54)/y - t^4.38*y + 3*t^8.54*y |
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 |
|---|---|---|---|---|---|---|---|---|
| 2153 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_2M_4$ + $ M_1M_4$ + $ M_1M_5$ + $ M_3M_4$ + $ M_3M_6$ | 0.658 | 0.8022 | 0.8202 | [X:[], M:[1.0769, 1.0769, 1.0769, 0.9231, 0.9231, 0.9231], q:[0.7692, 0.4615], qb:[0.4615, 0.4615], phi:[0.4615]] | 4*t^2.77 + 3*t^3.69 + 6*t^4.15 + 10*t^5.54 - 9*t^6. - t^4.38/y - t^4.38*y | detail | {a: 11565/17576, c: 3525/4394, M1: 14/13, M2: 14/13, M3: 14/13, M4: 12/13, M5: 12/13, M6: 12/13, q1: 10/13, q2: 6/13, qb1: 6/13, qb2: 6/13, phi1: 6/13} |
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 693 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_2M_4$ + $ M_1M_4$ + $ M_1M_5$ | 0.6566 | 0.7988 | 0.822 | [X:[], M:[1.0916, 1.0916, 0.9962, 0.9084, 0.9084], q:[0.7729, 0.4065], qb:[0.5019, 0.5019], phi:[0.4542]] | 3*t^2.73 + t^2.99 + t^3.54 + t^3.8 + 2*t^3.82 + 2*t^4.09 + 3*t^4.37 + 6*t^5.45 + t^5.71 + t^5.98 - 5*t^6. - t^4.36/y - t^4.36*y | detail |