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 |
|---|---|---|---|---|---|---|---|---|---|
| 3290 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_4\phi_1q_2^2$ + $ M_5q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ + $ M_6\phi_1q_2\tilde{q}_2$ | 0.6259 | 0.8118 | 0.771 | [X:[], M:[1.0, 1.0259, 0.9482, 1.0259, 0.7306, 0.7306], q:[0.7565, 0.2435], qb:[0.513, 0.5389], phi:[0.487]] | [X:[], M:[[0], [4], [-8], [4], [-3], [-3]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ M_6$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ M_3$, $ M_1$, $ M_2$, $ M_4$, $ \phi_1q_2\tilde{q}_1$, $ q_1\tilde{q}_2$, $ M_5^2$, $ M_5M_6$, $ M_6^2$, $ \phi_1q_1q_2$, $ M_5q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ M_5q_2\tilde{q}_2$, $ M_6q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_2^2$, $ M_3M_5$, $ M_3M_6$, $ M_1M_5$, $ M_1M_6$, $ M_2M_5$, $ M_4M_5$, $ M_2M_6$, $ M_4M_6$, $ \phi_1q_1\tilde{q}_1$, $ M_2q_2\tilde{q}_1$, $ M_4q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_2q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_2$, $ M_3^2$, $ M_1M_3$, $ M_2M_3$, $ M_3M_4$, $ M_5\phi_1q_2\tilde{q}_1$, $ M_6\phi_1q_2\tilde{q}_1$ | $\phi_1q_2^2\tilde{q}_1^2$ | -2 | 2*t^2.19 + t^2.27 + t^2.35 + t^2.84 + t^3. + 2*t^3.08 + t^3.73 + t^3.89 + 3*t^4.38 + 2*t^4.46 + 4*t^4.54 + 2*t^4.62 + 2*t^4.69 + 2*t^5.04 + 2*t^5.19 + 5*t^5.27 + 3*t^5.35 + 2*t^5.42 + t^5.69 + t^5.84 + 2*t^5.92 - 2*t^6. + 3*t^6.08 + 3*t^6.16 + t^6.23 + 4*t^6.58 + t^6.65 + 6*t^6.73 + 4*t^6.81 + 5*t^6.89 + 4*t^6.96 + 2*t^7.04 + 3*t^7.23 + 3*t^7.38 + 6*t^7.46 + 4*t^7.54 + 7*t^7.62 + 4*t^7.69 + 4*t^7.77 + 2*t^7.88 + 2*t^8.04 + 3*t^8.11 - 6*t^8.19 + t^8.27 + 2*t^8.35 + 5*t^8.42 + 3*t^8.5 + t^8.53 + 2*t^8.58 + t^8.69 + 6*t^8.77 - 2*t^8.84 + 7*t^8.92 - t^4.46/y - (2*t^6.65)/y - t^7.31/y + (2*t^7.38)/y + (2*t^7.46)/y + t^7.54/y + (2*t^7.62)/y + (2*t^8.04)/y + t^8.11/y + (3*t^8.19)/y + (7*t^8.27)/y + (3*t^8.35)/y + (2*t^8.42)/y - (2*t^8.84)/y + (4*t^8.92)/y - t^4.46*y - 2*t^6.65*y - t^7.31*y + 2*t^7.38*y + 2*t^7.46*y + t^7.54*y + 2*t^7.62*y + 2*t^8.04*y + t^8.11*y + 3*t^8.19*y + 7*t^8.27*y + 3*t^8.35*y + 2*t^8.42*y - 2*t^8.84*y + 4*t^8.92*y | (2*t^2.19)/g1^3 + g1*t^2.27 + g1^5*t^2.35 + t^2.84/g1^8 + t^3. + 2*g1^4*t^3.08 + t^3.73/g1 + g1^7*t^3.89 + (3*t^4.38)/g1^6 + (2*t^4.46)/g1^2 + 4*g1^2*t^4.54 + 2*g1^6*t^4.62 + 2*g1^10*t^4.69 + (2*t^5.04)/g1^11 + (2*t^5.19)/g1^3 + 5*g1*t^5.27 + 3*g1^5*t^5.35 + 2*g1^9*t^5.42 + t^5.69/g1^16 + t^5.84/g1^8 + (2*t^5.92)/g1^4 - 2*t^6. + 3*g1^4*t^6.08 + 3*g1^8*t^6.16 + g1^12*t^6.23 + (4*t^6.58)/g1^9 + t^6.65/g1^5 + (6*t^6.73)/g1 + 4*g1^3*t^6.81 + 5*g1^7*t^6.89 + 4*g1^11*t^6.96 + 2*g1^15*t^7.04 + (3*t^7.23)/g1^14 + (3*t^7.38)/g1^6 + (6*t^7.46)/g1^2 + 4*g1^2*t^7.54 + 7*g1^6*t^7.62 + 4*g1^10*t^7.69 + 4*g1^14*t^7.77 + (2*t^7.88)/g1^19 + (2*t^8.04)/g1^11 + (3*t^8.11)/g1^7 - (6*t^8.19)/g1^3 + g1*t^8.27 + 2*g1^5*t^8.35 + 5*g1^9*t^8.42 + 3*g1^13*t^8.5 + t^8.53/g1^24 + 2*g1^17*t^8.58 + t^8.69/g1^16 + (6*t^8.77)/g1^12 - (2*t^8.84)/g1^8 + (7*t^8.92)/g1^4 - t^4.46/(g1^2*y) - (2*t^6.65)/(g1^5*y) - t^7.31/(g1^10*y) + (2*t^7.38)/(g1^6*y) + (2*t^7.46)/(g1^2*y) + (g1^2*t^7.54)/y + (2*g1^6*t^7.62)/y + (2*t^8.04)/(g1^11*y) + t^8.11/(g1^7*y) + (3*t^8.19)/(g1^3*y) + (7*g1*t^8.27)/y + (3*g1^5*t^8.35)/y + (2*g1^9*t^8.42)/y - (2*t^8.84)/(g1^8*y) + (4*t^8.92)/(g1^4*y) - (t^4.46*y)/g1^2 - (2*t^6.65*y)/g1^5 - (t^7.31*y)/g1^10 + (2*t^7.38*y)/g1^6 + (2*t^7.46*y)/g1^2 + g1^2*t^7.54*y + 2*g1^6*t^7.62*y + (2*t^8.04*y)/g1^11 + (t^8.11*y)/g1^7 + (3*t^8.19*y)/g1^3 + 7*g1*t^8.27*y + 3*g1^5*t^8.35*y + 2*g1^9*t^8.42*y - (2*t^8.84*y)/g1^8 + (4*t^8.92*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2776 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_4\phi_1q_2^2$ + $ M_5q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ | 0.6062 | 0.7757 | 0.7814 | [X:[], M:[1.0, 1.0213, 0.9574, 1.0213, 0.734], q:[0.7553, 0.2447], qb:[0.5106, 0.5319], phi:[0.4894]] | t^2.2 + t^2.27 + t^2.33 + t^2.87 + t^3. + 2*t^3.06 + t^3.73 + t^3.8 + t^3.86 + t^4.4 + t^4.47 + 3*t^4.53 + 2*t^4.6 + 2*t^4.66 + t^5.07 + t^5.2 + 3*t^5.27 + 3*t^5.33 + 2*t^5.39 + t^5.74 + t^5.87 + t^5.94 - t^6. - t^4.47/y - t^4.47*y | detail |