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 |
|---|---|---|---|---|---|---|---|---|---|
| 56107 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_2q_1\tilde{q}_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_4q_1q_2$ + $ M_1M_5$ + $ M_6q_1\tilde{q}_1$ + $ M_7\phi_1q_2^2$ | 0.6984 | 0.9171 | 0.7615 | [X:[], M:[1.125, 0.75, 0.75, 0.875, 0.875, 0.875, 0.75], q:[0.75, 0.375], qb:[0.375, 0.5], phi:[0.5]] | [X:[], M:[[1], [0], [-2], [1], [-1], [-1], [2]], q:[[0], [-1]], qb:[[1], [0]], phi:[[0]]] | 1 | {a: 5721/8192, c: 7513/8192, M1: 9/8, M2: 3/4, M3: 3/4, M4: 7/8, M5: 7/8, M6: 7/8, M7: 3/4, q1: 3/4, q2: 3/8, qb1: 3/8, qb2: 1/2, phi1: 1/2} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ M_3$, $ M_7$, $ q_2\tilde{q}_1$, $ M_3$, $ M_7$, $ M_5$, $ M_6$, $ M_4$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1^2$, $ q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2^2$, $ M_2M_3$, $ M_3^2$, $ M_2M_7$, $ M_3M_7$, $ M_7^2$, $ M_2q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_1$, $ M_7q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ \phi_1\tilde{q}_2^2$, $ M_3^2$, $ M_2M_3$, $ M_3q_2\tilde{q}_1$, $ M_2M_7$, $ M_7q_2\tilde{q}_1$, $ M_7^2$, $ M_3M_5$, $ M_3M_6$, $ M_3M_4$, $ M_2M_5$, $ M_2M_6$, $ M_5q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ M_3\tilde{q}_1\tilde{q}_2$, $ M_2M_4$, $ M_5M_7$, $ M_6M_7$, $ M_4q_2\tilde{q}_1$, $ M_2\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_4M_7$, $ M_7\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ M_4M_5$, $ M_5^2$, $ M_4M_6$, $ M_5M_6$, $ M_6^2$, $ M_2\phi_1^2$, $ M_3\phi_1^2$, $ M_7\phi_1^2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_5\tilde{q}_1\tilde{q}_2$, $ M_6\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_5^2$, $ M_5M_6$, $ M_6^2$, $ M_3\phi_1^2$, $ M_4^2$, $ M_7\phi_1^2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_5\phi_1^2$, $ M_6\phi_1^2$, $ M_4\phi_1^2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$ | $M_3q_1\tilde{q}_2$, $ M_7q_1\tilde{q}_2$ | -1 | 4*t^2.25 + 4*t^2.62 + t^3. + t^3.75 + 2*t^4.12 + 11*t^4.5 + 16*t^4.88 + 14*t^5.25 + 2*t^5.62 - t^6. + 6*t^6.38 + 27*t^6.75 + 38*t^7.12 + 42*t^7.5 + 22*t^7.88 - 8*t^8.25 - 8*t^8.62 - t^4.5/y - (3*t^6.75)/y - (2*t^7.12)/y + (6*t^7.5)/y + (18*t^7.88)/y + (13*t^8.25)/y + (4*t^8.62)/y - t^4.5*y - 3*t^6.75*y - 2*t^7.12*y + 6*t^7.5*y + 18*t^7.88*y + 13*t^8.25*y + 4*t^8.62*y | 2*t^2.25 + t^2.25/g1^2 + g1^2*t^2.25 + (2*t^2.62)/g1 + 2*g1*t^2.62 + t^3. + t^3.75 + t^4.12/g1 + g1*t^4.12 + 5*t^4.5 + t^4.5/g1^4 + (2*t^4.5)/g1^2 + 2*g1^2*t^4.5 + g1^4*t^4.5 + (2*t^4.88)/g1^3 + (6*t^4.88)/g1 + 6*g1*t^4.88 + 2*g1^3*t^4.88 + 6*t^5.25 + (4*t^5.25)/g1^2 + 4*g1^2*t^5.25 + t^5.62/g1 + g1*t^5.62 - t^6. + t^6.38/g1^3 + (2*t^6.38)/g1 + 2*g1*t^6.38 + g1^3*t^6.38 + 9*t^6.75 + t^6.75/g1^6 + (2*t^6.75)/g1^4 + (6*t^6.75)/g1^2 + 6*g1^2*t^6.75 + 2*g1^4*t^6.75 + g1^6*t^6.75 + (2*t^7.12)/g1^5 + (6*t^7.12)/g1^3 + (11*t^7.12)/g1 + 11*g1*t^7.12 + 6*g1^3*t^7.12 + 2*g1^5*t^7.12 + 14*t^7.5 + (4*t^7.5)/g1^4 + (10*t^7.5)/g1^2 + 10*g1^2*t^7.5 + 4*g1^4*t^7.5 + (5*t^7.88)/g1^3 + (6*t^7.88)/g1 + 6*g1*t^7.88 + 5*g1^3*t^7.88 - 4*t^8.25 - (2*t^8.25)/g1^2 - 2*g1^2*t^8.25 + t^8.62/g1^5 - (5*t^8.62)/g1 - 5*g1*t^8.62 + g1^5*t^8.62 - t^4.5/y - t^6.75/y - t^6.75/(g1^2*y) - (g1^2*t^6.75)/y - t^7.12/(g1*y) - (g1*t^7.12)/y + (2*t^7.5)/y + (2*t^7.5)/(g1^2*y) + (2*g1^2*t^7.5)/y + (2*t^7.88)/(g1^3*y) + (7*t^7.88)/(g1*y) + (7*g1*t^7.88)/y + (2*g1^3*t^7.88)/y + (7*t^8.25)/y + (3*t^8.25)/(g1^2*y) + (3*g1^2*t^8.25)/y + (2*t^8.62)/(g1*y) + (2*g1*t^8.62)/y - t^4.5*y - t^6.75*y - (t^6.75*y)/g1^2 - g1^2*t^6.75*y - (t^7.12*y)/g1 - g1*t^7.12*y + 2*t^7.5*y + (2*t^7.5*y)/g1^2 + 2*g1^2*t^7.5*y + (2*t^7.88*y)/g1^3 + (7*t^7.88*y)/g1 + 7*g1*t^7.88*y + 2*g1^3*t^7.88*y + 7*t^8.25*y + (3*t^8.25*y)/g1^2 + 3*g1^2*t^8.25*y + (2*t^8.62*y)/g1 + 2*g1*t^8.62*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 50953 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_2q_1\tilde{q}_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_4q_1q_2$ + $ M_1M_5$ + $ M_6q_1\tilde{q}_1$ | 0.6798 | 0.8846 | 0.7686 | [X:[], M:[1.1378, 0.75, 0.7244, 0.8878, 0.8622, 0.8622], q:[0.75, 0.3622], qb:[0.3878, 0.5], phi:[0.5]] | t^2.17 + 2*t^2.25 + 2*t^2.59 + 2*t^2.66 + t^3. + t^3.67 + t^3.75 + t^4.09 + t^4.16 + t^4.35 + 2*t^4.42 + 4*t^4.5 + 2*t^4.76 + 6*t^4.84 + 4*t^4.91 + 4*t^5.17 + 6*t^5.25 + 3*t^5.33 + t^5.59 + t^5.66 + t^5.85 + 2*t^5.92 - t^6. - t^4.5/y - t^4.5*y | detail |