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 |
|---|---|---|---|---|---|---|---|---|---|
| 56483 | SU2adj1nf2 | $M_1\phi_1^2$ + $ M_2q_1q_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_2M_4$ + $ M_5q_1\tilde{q}_2$ + $ M_5q_2\tilde{q}_2$ + $ M_5M_6$ + $ M_2M_7$ | 0.6624 | 0.7901 | 0.8384 | [X:[], M:[1.1553, 1.0435, 0.9565, 0.9565, 0.7329, 1.2671, 0.9565], q:[0.4782, 0.4782], qb:[0.5653, 0.7888], phi:[0.4224]] | [X:[], M:[[4], [14], [-14], [-14], [6], [-6], [-14]], q:[[-7], [-7]], qb:[[21], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ M_4$, $ M_7$, $ M_1$, $ M_6$, $ q_2\tilde{q}_2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_1^2$, $ \phi_1q_1q_2$, $ \phi_1q_2^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_3^2$, $ M_3M_4$, $ M_4^2$, $ M_3M_7$, $ M_4M_7$, $ M_7^2$ | . | -5 | 3*t^2.87 + t^3.47 + 2*t^3.8 + t^4.06 + 3*t^4.14 + 2*t^4.4 + t^4.66 + 4*t^5.74 - 5*t^6. - 2*t^6.26 + t^6.34 - t^6.6 + 5*t^6.67 + t^6.93 + 7*t^7.01 + 2*t^7.27 + t^7.53 + 3*t^7.6 + 2*t^7.86 + 4*t^7.94 + t^8.12 + 3*t^8.2 + 5*t^8.27 + 2*t^8.46 + 2*t^8.53 + 5*t^8.61 + t^8.72 + 2*t^8.8 - 13*t^8.87 - t^4.27/y - (2*t^7.14)/y + (2*t^7.4)/y + (3*t^8.74)/y - t^4.27*y - 2*t^7.14*y + 2*t^7.4*y + 3*t^8.74*y | (3*t^2.87)/g1^14 + g1^4*t^3.47 + (2*t^3.8)/g1^6 + g1^22*t^4.06 + (3*t^4.14)/g1^16 + 2*g1^12*t^4.4 + g1^40*t^4.66 + (4*t^5.74)/g1^28 - 5*t^6. - 2*g1^28*t^6.26 + t^6.34/g1^10 - g1^18*t^6.6 + (5*t^6.67)/g1^20 + g1^8*t^6.93 + (7*t^7.01)/g1^30 + (2*t^7.27)/g1^2 + g1^26*t^7.53 + (3*t^7.6)/g1^12 + 2*g1^16*t^7.86 + (4*t^7.94)/g1^22 + g1^44*t^8.12 + 3*g1^6*t^8.2 + (5*t^8.27)/g1^32 + 2*g1^34*t^8.46 + (2*t^8.53)/g1^4 + (5*t^8.61)/g1^42 + g1^62*t^8.72 + 2*g1^24*t^8.8 - (13*t^8.87)/g1^14 - t^4.27/(g1^2*y) - (2*t^7.14)/(g1^16*y) + (2*g1^12*t^7.4)/y + (3*t^8.74)/(g1^28*y) - (t^4.27*y)/g1^2 - (2*t^7.14*y)/g1^16 + 2*g1^12*t^7.4*y + (3*t^8.74*y)/g1^28 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 53409 | SU2adj1nf2 | $M_1\phi_1^2$ + $ M_2q_1q_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_2M_4$ + $ M_5q_1\tilde{q}_2$ + $ M_5q_2\tilde{q}_2$ + $ M_5M_6$ | 0.6593 | 0.7843 | 0.8406 | [X:[], M:[1.1493, 1.0225, 0.9775, 0.9775, 0.7239, 1.2761], q:[0.4887, 0.4887], qb:[0.5338, 0.7873], phi:[0.4254]] | 2*t^2.93 + t^3.07 + t^3.45 + 2*t^3.83 + t^3.96 + 3*t^4.21 + 2*t^4.34 + t^4.48 + t^5.86 - 3*t^6. - t^4.28/y - t^4.28*y | detail |