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 |
|---|---|---|---|---|---|---|---|---|---|
| 3133 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_3M_5$ + $ M_2\phi_1^2$ + $ M_6\phi_1^2$ + $ \phi_1q_2^2$ + $ M_7\phi_1q_1\tilde{q}_1$ | 0.69 | 0.8775 | 0.7863 | [X:[], M:[0.8342, 1.0553, 1.1658, 0.7237, 0.8342, 1.0553, 0.6934], q:[0.402, 0.7638], qb:[0.4323, 0.5125], phi:[0.4724]] | [X:[], M:[[-12], [4], [12], [-20], [-12], [4], [14]], q:[[11], [1]], qb:[[-23], [19]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_7$, $ M_4$, $ M_1$, $ M_5$, $ q_1\tilde{q}_2$, $ M_2$, $ M_6$, $ q_2\tilde{q}_1$, $ \phi_1q_1^2$, $ \phi_1\tilde{q}_1^2$, $ M_7^2$, $ \phi_1q_1\tilde{q}_2$, $ M_4M_7$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ \phi_1\tilde{q}_2^2$, $ M_1M_7$, $ M_5M_7$, $ M_1M_4$, $ M_4M_5$, $ M_7q_1\tilde{q}_2$, $ \phi_1q_1q_2$, $ M_4q_1\tilde{q}_2$, $ M_1^2$, $ M_1M_5$, $ M_5^2$, $ \phi_1q_2\tilde{q}_1$, $ M_2M_7$, $ M_6M_7$, $ M_5q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ M_2M_4$, $ M_4M_6$, $ q_1^2\tilde{q}_2^2$, $ M_1M_2$, $ M_2M_5$, $ M_1M_6$, $ M_5M_6$, $ M_7q_2\tilde{q}_1$, $ M_7\phi_1q_1^2$, $ M_6q_1\tilde{q}_2$ | $M_4\phi_1q_1^2$ | -2 | t^2.08 + t^2.17 + 2*t^2.5 + t^2.74 + 2*t^3.17 + t^3.59 + t^3.83 + t^4.01 + 2*t^4.16 + 2*t^4.25 + t^4.34 + t^4.49 + 2*t^4.58 + 2*t^4.67 + t^4.82 + t^4.91 + 3*t^5.01 + 4*t^5.25 + 2*t^5.34 + t^5.49 + 4*t^5.67 + 2*t^5.91 - 2*t^6. + 2*t^6.09 + t^6.18 + t^6.24 + 6*t^6.33 + t^6.42 + 3*t^6.51 + 2*t^6.57 + 3*t^6.66 + 5*t^6.75 + 2*t^6.85 + 2*t^6.9 + 3*t^6.99 + t^7.09 + 4*t^7.18 + t^7.24 + 4*t^7.33 + 3*t^7.42 + 4*t^7.51 + t^7.57 + t^7.6 + t^7.66 + 5*t^7.75 + 3*t^7.84 + 4*t^7.99 + t^8.02 - 2*t^8.08 + 3*t^8.17 + t^8.23 + t^8.26 + 2*t^8.32 + t^8.35 + 5*t^8.41 - t^8.5 + 4*t^8.59 + 4*t^8.65 + 3*t^8.68 + 8*t^8.83 + 2*t^8.93 + 2*t^8.98 - t^4.42/y - t^6.5/y - t^6.59/y - t^6.92/y + (2*t^7.25)/y + t^7.58/y + (2*t^7.67)/y + t^7.82/y + (2*t^7.91)/y + t^8.01/y + (5*t^8.25)/y + (3*t^8.34)/y - t^8.58/y + (4*t^8.67)/y + (3*t^8.91)/y - t^4.42*y - t^6.5*y - t^6.59*y - t^6.92*y + 2*t^7.25*y + t^7.58*y + 2*t^7.67*y + t^7.82*y + 2*t^7.91*y + t^8.01*y + 5*t^8.25*y + 3*t^8.34*y - t^8.58*y + 4*t^8.67*y + 3*t^8.91*y | g1^14*t^2.08 + t^2.17/g1^20 + (2*t^2.5)/g1^12 + g1^30*t^2.74 + 2*g1^4*t^3.17 + t^3.59/g1^22 + g1^20*t^3.83 + t^4.01/g1^48 + 2*g1^28*t^4.16 + (2*t^4.25)/g1^6 + t^4.34/g1^40 + g1^36*t^4.49 + 2*g1^2*t^4.58 + (2*t^4.67)/g1^32 + g1^44*t^4.82 + g1^10*t^4.91 + (3*t^5.01)/g1^24 + 4*g1^18*t^5.25 + (2*t^5.34)/g1^16 + g1^60*t^5.49 + (4*t^5.67)/g1^8 + 2*g1^34*t^5.91 - 2*t^6. + (2*t^6.09)/g1^34 + t^6.18/g1^68 + g1^42*t^6.24 + 6*g1^8*t^6.33 + t^6.42/g1^26 + (3*t^6.51)/g1^60 + 2*g1^50*t^6.57 + 3*g1^16*t^6.66 + (5*t^6.75)/g1^18 + (2*t^6.85)/g1^52 + 2*g1^58*t^6.9 + 3*g1^24*t^6.99 + t^7.09/g1^10 + (4*t^7.18)/g1^44 + g1^66*t^7.24 + 4*g1^32*t^7.33 + (3*t^7.42)/g1^2 + (4*t^7.51)/g1^36 + g1^74*t^7.57 + t^7.6/g1^70 + g1^40*t^7.66 + 5*g1^6*t^7.75 + (3*t^7.84)/g1^28 + 4*g1^48*t^7.99 + t^8.02/g1^96 - 2*g1^14*t^8.08 + (3*t^8.17)/g1^20 + g1^90*t^8.23 + t^8.26/g1^54 + 2*g1^56*t^8.32 + t^8.35/g1^88 + 5*g1^22*t^8.41 - t^8.5/g1^12 + (4*t^8.59)/g1^46 + 4*g1^64*t^8.65 + (3*t^8.68)/g1^80 + (8*t^8.83)/g1^4 + (2*t^8.93)/g1^38 + 2*g1^72*t^8.98 - t^4.42/(g1^2*y) - (g1^12*t^6.5)/y - t^6.59/(g1^22*y) - t^6.92/(g1^14*y) + (2*t^7.25)/(g1^6*y) + (g1^2*t^7.58)/y + (2*t^7.67)/(g1^32*y) + (g1^44*t^7.82)/y + (2*g1^10*t^7.91)/y + t^8.01/(g1^24*y) + (5*g1^18*t^8.25)/y + (3*t^8.34)/(g1^16*y) - (g1^26*t^8.58)/y + (4*t^8.67)/(g1^8*y) + (3*g1^34*t^8.91)/y - (t^4.42*y)/g1^2 - g1^12*t^6.5*y - (t^6.59*y)/g1^22 - (t^6.92*y)/g1^14 + (2*t^7.25*y)/g1^6 + g1^2*t^7.58*y + (2*t^7.67*y)/g1^32 + g1^44*t^7.82*y + 2*g1^10*t^7.91*y + (t^8.01*y)/g1^24 + 5*g1^18*t^8.25*y + (3*t^8.34*y)/g1^16 - g1^26*t^8.58*y + (4*t^8.67*y)/g1^8 + 3*g1^34*t^8.91*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2063 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_3M_5$ + $ M_2\phi_1^2$ + $ M_6\phi_1^2$ + $ \phi_1q_2^2$ | 0.6694 | 0.8378 | 0.799 | [X:[], M:[0.8331, 1.0556, 1.1669, 0.7218, 0.8331, 1.0556], q:[0.403, 0.7639], qb:[0.4301, 0.5143], phi:[0.4722]] | t^2.17 + 2*t^2.5 + t^2.75 + 2*t^3.17 + t^3.58 + t^3.83 + t^3.92 + t^4. + t^4.17 + t^4.25 + t^4.33 + t^4.5 + 2*t^4.66 + t^4.92 + 3*t^5. + 2*t^5.25 + 2*t^5.33 + t^5.5 + 3*t^5.67 + t^5.92 - 2*t^6. - t^4.42/y - t^4.42*y | detail |