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 |
|---|---|---|---|---|---|---|---|---|---|
| 2915 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_1$ | 0.5776 | 0.7619 | 0.758 | [X:[], M:[1.0501, 0.8497, 0.9499, 1.1503, 0.6753, 0.7495], q:[0.7625, 0.1874], qb:[0.6623, 0.4879], phi:[0.475]] | [X:[], M:[[4], [-12], [-4], [12], [14], [-20]], q:[[1], [-5]], qb:[[-7], [19]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ q_2\tilde{q}_2$, $ M_6$, $ \phi_1q_2^2$, $ q_2\tilde{q}_1$, $ M_3$, $ \phi_1^2$, $ M_4$, $ \phi_1q_2\tilde{q}_2$, $ M_5^2$, $ M_5q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_5M_6$, $ \phi_1q_1q_2$, $ q_1\tilde{q}_1$, $ M_6q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_6^2$, $ M_5\phi_1q_2^2$, $ M_5q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_6\phi_1q_2^2$, $ M_6q_2\tilde{q}_1$, $ M_3M_5$, $ M_5\phi_1^2$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3M_6$, $ M_6\phi_1^2$, $ \phi_1^2q_2^4$, $ \phi_1q_2^3\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_3\phi_1q_2^2$, $ \phi_1^3q_2^2$, $ M_3q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_4M_5$, $ M_4q_2\tilde{q}_2$, $ M_5\phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_2^2$, $ M_3^2$, $ M_4M_6$, $ M_3\phi_1^2$, $ \phi_1^4$, $ \phi_1q_1\tilde{q}_1$, $ M_6\phi_1q_2\tilde{q}_2$ | $M_4\phi_1q_2^2$, $ \phi_1^2q_2^3\tilde{q}_2$ | -1 | 2*t^2.03 + t^2.25 + 2*t^2.55 + 2*t^2.85 + 2*t^3.45 + 3*t^4.05 + 3*t^4.27 + t^4.35 + t^4.5 + 3*t^4.58 + 2*t^4.8 + 5*t^4.88 + 4*t^5.1 + 5*t^5.4 + 3*t^5.48 + 3*t^5.7 - t^6. + 4*t^6.08 + 6*t^6.3 + 2*t^6.38 + t^6.52 + 3*t^6.6 + t^6.75 + 3*t^6.82 + 9*t^6.9 + 2*t^7.05 + 7*t^7.12 + t^7.2 + 4*t^7.35 + 4*t^7.42 + 3*t^7.5 + 7*t^7.65 + 6*t^7.73 + 2*t^7.8 + 7*t^7.95 - 5*t^8.03 + 5*t^8.1 + 2*t^8.25 + 7*t^8.33 + 3*t^8.4 - t^8.55 + 3*t^8.63 + t^8.7 + t^8.77 - 3*t^8.85 + 11*t^8.93 + t^8.99 - t^4.42/y - t^6.45/y - t^6.67/y + t^7.05/y + t^7.27/y + (5*t^7.58)/y + (2*t^7.8)/y + (4*t^7.88)/y + (3*t^8.1)/y + t^8.18/y + (5*t^8.4)/y + (3*t^8.48)/y + (2*t^8.7)/y - t^8.92/y - t^4.42*y - t^6.45*y - t^6.67*y + t^7.05*y + t^7.27*y + 5*t^7.58*y + 2*t^7.8*y + 4*t^7.88*y + 3*t^8.1*y + t^8.18*y + 5*t^8.4*y + 3*t^8.48*y + 2*t^8.7*y - t^8.92*y | 2*g1^14*t^2.03 + t^2.25/g1^20 + (2*t^2.55)/g1^12 + (2*t^2.85)/g1^4 + 2*g1^12*t^3.45 + 3*g1^28*t^4.05 + (3*t^4.27)/g1^6 + g1^36*t^4.35 + t^4.5/g1^40 + 3*g1^2*t^4.58 + (2*t^4.8)/g1^32 + 5*g1^10*t^4.88 + (4*t^5.1)/g1^24 + (5*t^5.4)/g1^16 + 3*g1^26*t^5.48 + (3*t^5.7)/g1^8 - t^6. + 4*g1^42*t^6.08 + 6*g1^8*t^6.3 + 2*g1^50*t^6.38 + t^6.52/g1^26 + 3*g1^16*t^6.6 + t^6.75/g1^60 + (3*t^6.82)/g1^18 + 9*g1^24*t^6.9 + (2*t^7.05)/g1^52 + (7*t^7.12)/g1^10 + g1^32*t^7.2 + (4*t^7.35)/g1^44 + (4*t^7.42)/g1^2 + 3*g1^40*t^7.5 + (7*t^7.65)/g1^36 + 6*g1^6*t^7.73 + 2*g1^48*t^7.8 + (7*t^7.95)/g1^28 - 5*g1^14*t^8.03 + 5*g1^56*t^8.1 + (2*t^8.25)/g1^20 + 7*g1^22*t^8.33 + 3*g1^64*t^8.4 - t^8.55/g1^12 + 3*g1^30*t^8.63 + g1^72*t^8.7 + t^8.77/g1^46 - (3*t^8.85)/g1^4 + 11*g1^38*t^8.93 + t^8.99/g1^80 - t^4.42/(g1^2*y) - (g1^12*t^6.45)/y - t^6.67/(g1^22*y) + (g1^28*t^7.05)/y + t^7.27/(g1^6*y) + (5*g1^2*t^7.58)/y + (2*t^7.8)/(g1^32*y) + (4*g1^10*t^7.88)/y + (3*t^8.1)/(g1^24*y) + (g1^18*t^8.18)/y + (5*t^8.4)/(g1^16*y) + (3*g1^26*t^8.48)/y + (2*t^8.7)/(g1^8*y) - t^8.92/(g1^42*y) - (t^4.42*y)/g1^2 - g1^12*t^6.45*y - (t^6.67*y)/g1^22 + g1^28*t^7.05*y + (t^7.27*y)/g1^6 + 5*g1^2*t^7.58*y + (2*t^7.8*y)/g1^32 + 4*g1^10*t^7.88*y + (3*t^8.1*y)/g1^24 + g1^18*t^8.18*y + (5*t^8.4*y)/g1^16 + 3*g1^26*t^8.48*y + (2*t^8.7*y)/g1^8 - (t^8.92*y)/g1^42 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1893 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1\tilde{q}_2$ | 0.6295 | 0.8188 | 0.7688 | [X:[], M:[0.9716, 1.0851, 1.0284, 0.9149, 0.7478, 0.7947], q:[0.7429, 0.2855], qb:[0.4525, 0.4624], phi:[0.5142]] | t^2.21 + 2*t^2.24 + t^2.38 + t^2.74 + 2*t^3.09 + t^3.26 + t^3.59 + t^3.79 + t^4.26 + t^4.29 + t^4.32 + t^4.43 + 2*t^4.46 + 3*t^4.49 + t^4.6 + 2*t^4.63 + t^4.77 + t^4.96 + 2*t^4.99 + t^5.13 + 2*t^5.3 + 4*t^5.33 + 2*t^5.47 + t^5.49 + t^5.5 + t^5.64 + t^5.8 + 3*t^5.83 - 2*t^6. - t^4.54/y - t^4.54*y | detail |