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 |
|---|---|---|---|---|---|---|---|---|---|
| 56163 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_5q_2\tilde{q}_1$ + $ M_2^2$ + $ M_6\phi_1q_1^2$ + $ M_1M_6$ + $ M_7\phi_1q_1q_2$ | 0.7051 | 0.8954 | 0.7874 | [X:[], M:[1.11, 1.0, 0.89, 0.688, 0.798, 0.89, 0.688], q:[0.344, 0.546], qb:[0.656, 0.766], phi:[0.422]] | [X:[], M:[[5], [0], [-5], [4], [9], [-5], [4]], q:[[2], [-7]], qb:[[-2], [3]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_7$, $ M_5$, $ \phi_1^2$, $ M_3$, $ M_6$, $ M_2$, $ M_1$, $ M_4^2$, $ M_4M_7$, $ M_7^2$, $ \phi_1q_1\tilde{q}_1$, $ \tilde{q}_1\tilde{q}_2$, $ M_4M_5$, $ M_5M_7$, $ \phi_1q_2^2$, $ M_4\phi_1^2$, $ M_7\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_3M_4$, $ M_4M_6$, $ M_3M_7$, $ M_6M_7$, $ M_5^2$, $ \phi_1q_2\tilde{q}_1$, $ M_5\phi_1^2$, $ M_2M_4$, $ M_3M_5$, $ M_5M_6$, $ M_2M_7$, $ \phi_1^4$, $ M_3\phi_1^2$, $ M_6\phi_1^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_3^2$, $ M_3M_6$, $ M_6^2$, $ M_1M_4$, $ M_2M_5$, $ M_1M_7$, $ M_2\phi_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1M_5$, $ M_1\phi_1^2$, $ \phi_1\tilde{q}_2^2$ | . | -2 | 2*t^2.06 + t^2.39 + t^2.53 + 2*t^2.67 + t^3. + t^3.33 + 3*t^4.13 + 2*t^4.27 + 2*t^4.46 + t^4.54 + 3*t^4.6 + 3*t^4.73 + t^4.79 + t^4.87 + t^4.93 + 4*t^5.06 + 4*t^5.2 + 2*t^5.34 + 2*t^5.39 + 2*t^5.53 + t^5.72 + 2*t^5.86 - 2*t^6. + 4*t^6.19 + 2*t^6.33 + 3*t^6.52 + 6*t^6.66 + 5*t^6.8 + 2*t^6.85 + 2*t^6.94 + 3*t^6.99 + t^7.07 + 7*t^7.13 + t^7.18 + 2*t^7.21 + 7*t^7.27 + t^7.32 + 3*t^7.4 + 5*t^7.46 + 2*t^7.54 + 8*t^7.6 + 3*t^7.73 + 2*t^7.79 + 4*t^7.87 + 5*t^7.93 + t^8.01 - 5*t^8.06 + t^8.12 + 7*t^8.26 - 2*t^8.34 + t^8.39 + t^8.53 + 4*t^8.59 - 8*t^8.67 + 7*t^8.72 + 7*t^8.86 + 3*t^8.92 - t^4.27/y - (2*t^6.33)/y - t^6.66/y - t^6.8/y - t^6.94/y + t^7.13/y + (2*t^7.46)/y + (3*t^7.6)/y + (5*t^7.73)/y + t^7.87/y + t^7.93/y + (4*t^8.06)/y + (4*t^8.2)/y + t^8.34/y + t^8.53/y + (2*t^8.67)/y - t^8.72/y - t^8.86/y - t^4.27*y - 2*t^6.33*y - t^6.66*y - t^6.8*y - t^6.94*y + t^7.13*y + 2*t^7.46*y + 3*t^7.6*y + 5*t^7.73*y + t^7.87*y + t^7.93*y + 4*t^8.06*y + 4*t^8.2*y + t^8.34*y + t^8.53*y + 2*t^8.67*y - t^8.72*y - t^8.86*y | 2*g1^4*t^2.06 + g1^9*t^2.39 + g1^2*t^2.53 + (2*t^2.67)/g1^5 + t^3. + g1^5*t^3.33 + 3*g1^8*t^4.13 + 2*g1*t^4.27 + 2*g1^13*t^4.46 + t^4.54/g1^13 + 3*g1^6*t^4.6 + (3*t^4.73)/g1 + g1^18*t^4.79 + t^4.87/g1^8 + g1^11*t^4.93 + 4*g1^4*t^5.06 + (4*t^5.2)/g1^3 + (2*t^5.34)/g1^10 + 2*g1^9*t^5.39 + 2*g1^2*t^5.53 + g1^14*t^5.72 + 2*g1^7*t^5.86 - 2*t^6. + 4*g1^12*t^6.19 + 2*g1^5*t^6.33 + 3*g1^17*t^6.52 + 6*g1^10*t^6.66 + 5*g1^3*t^6.8 + 2*g1^22*t^6.85 + (2*t^6.94)/g1^4 + 3*g1^15*t^6.99 + t^7.07/g1^11 + 7*g1^8*t^7.13 + g1^27*t^7.18 + (2*t^7.21)/g1^18 + 7*g1*t^7.27 + g1^20*t^7.32 + (3*t^7.4)/g1^6 + 5*g1^13*t^7.46 + (2*t^7.54)/g1^13 + 8*g1^6*t^7.6 + (3*t^7.73)/g1 + 2*g1^18*t^7.79 + (4*t^7.87)/g1^8 + 5*g1^11*t^7.93 + t^8.01/g1^15 - 5*g1^4*t^8.06 + g1^23*t^8.12 + 7*g1^16*t^8.26 - (2*t^8.34)/g1^10 + g1^9*t^8.39 + g1^2*t^8.53 + 4*g1^21*t^8.59 - (8*t^8.67)/g1^5 + 7*g1^14*t^8.72 + 7*g1^7*t^8.86 + 3*g1^26*t^8.92 - (g1*t^4.27)/y - (2*g1^5*t^6.33)/y - (g1^10*t^6.66)/y - (g1^3*t^6.8)/y - t^6.94/(g1^4*y) + (g1^8*t^7.13)/y + (2*g1^13*t^7.46)/y + (3*g1^6*t^7.6)/y + (5*t^7.73)/(g1*y) + t^7.87/(g1^8*y) + (g1^11*t^7.93)/y + (4*g1^4*t^8.06)/y + (4*t^8.2)/(g1^3*y) + t^8.34/(g1^10*y) + (g1^2*t^8.53)/y + (2*t^8.67)/(g1^5*y) - (g1^14*t^8.72)/y - (g1^7*t^8.86)/y - g1*t^4.27*y - 2*g1^5*t^6.33*y - g1^10*t^6.66*y - g1^3*t^6.8*y - (t^6.94*y)/g1^4 + g1^8*t^7.13*y + 2*g1^13*t^7.46*y + 3*g1^6*t^7.6*y + (5*t^7.73*y)/g1 + (t^7.87*y)/g1^8 + g1^11*t^7.93*y + 4*g1^4*t^8.06*y + (4*t^8.2*y)/g1^3 + (t^8.34*y)/g1^10 + g1^2*t^8.53*y + (2*t^8.67*y)/g1^5 - g1^14*t^8.72*y - g1^7*t^8.86*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50850 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_5q_2\tilde{q}_1$ + $ M_2^2$ + $ M_6\phi_1q_1^2$ + $ M_1M_6$ | 0.6844 | 0.8552 | 0.8003 | [X:[], M:[1.1117, 1.0, 0.8883, 0.6894, 0.8011, 0.8883], q:[0.3447, 0.5436], qb:[0.6553, 0.767], phi:[0.4223]] | t^2.07 + t^2.4 + t^2.53 + 2*t^2.66 + t^3. + t^3.34 + t^3.93 + t^4.14 + 2*t^4.27 + t^4.47 + t^4.53 + 2*t^4.6 + t^4.73 + t^4.81 + t^4.86 + t^4.94 + 3*t^5.07 + 4*t^5.2 + 2*t^5.33 + t^5.4 + 2*t^5.53 + t^5.74 + 2*t^5.87 - t^6. - t^4.27/y - t^4.27*y | detail |