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 |
|---|---|---|---|---|---|---|---|---|---|
| 46577 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ | 0.625 | 0.8119 | 0.7698 | [X:[], M:[0.9898, 0.7373, 0.778, 1.0305], q:[0.7475, 0.2627], qb:[0.4949, 0.4746], phi:[0.5051]] | [X:[], M:[[4], [5], [-11], [-12]], q:[[1], [-5]], qb:[[2], [10]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ M_3$, $ M_1$, $ \phi_1^2$, $ M_4$, $ \phi_1q_2^2$, $ q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_2^2$, $ M_2q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_2q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_2M_3$, $ \phi_1q_1q_2$, $ q_2^2\tilde{q}_1^2$, $ M_3q_2\tilde{q}_2$, $ M_3q_2\tilde{q}_1$, $ M_3^2$, $ M_1M_2$, $ \phi_1q_1\tilde{q}_2$, $ M_2\phi_1^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_2$, $ M_1M_3$, $ M_2M_4$, $ M_2\phi_1q_2^2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_4q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_3\phi_1^2$, $ M_4q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_3M_4$, $ M_3\phi_1q_2^2$, $ M_1^2$, $ M_2q_1\tilde{q}_1$, $ M_2\phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_2^2$ | . | -1 | 2*t^2.21 + t^2.27 + t^2.33 + t^2.97 + t^3.03 + 2*t^3.09 + 2*t^3.73 + t^4.36 + 4*t^4.42 + 3*t^4.48 + 3*t^4.55 + t^4.61 + t^4.67 + 2*t^5.18 + 3*t^5.24 + 5*t^5.3 + 2*t^5.36 + 2*t^5.43 + 3*t^5.94 - t^6. + 2*t^6.06 + 2*t^6.12 + 3*t^6.18 + 2*t^6.57 + 5*t^6.64 + 5*t^6.7 + 5*t^6.76 + 5*t^6.82 + 2*t^6.88 + t^6.94 + t^7. + 3*t^7.39 + 6*t^7.45 + 7*t^7.52 + 5*t^7.58 + 6*t^7.64 + 2*t^7.7 + 2*t^7.76 + t^8.09 + 2*t^8.15 - 4*t^8.21 + t^8.27 + t^8.33 + 7*t^8.39 + 3*t^8.46 + 3*t^8.52 + t^8.73 + 4*t^8.79 + 7*t^8.85 + 6*t^8.91 + 3*t^8.97 - t^4.52/y - t^6.73/y - t^6.85/y + (2*t^7.42)/y + (2*t^7.48)/y + (2*t^7.55)/y + (3*t^8.18)/y + (3*t^8.24)/y + (7*t^8.3)/y + (3*t^8.36)/y + (2*t^8.43)/y + (3*t^8.94)/y - t^4.52*y - t^6.73*y - t^6.85*y + 2*t^7.42*y + 2*t^7.48*y + 2*t^7.55*y + 3*t^8.18*y + 3*t^8.24*y + 7*t^8.3*y + 3*t^8.36*y + 2*t^8.43*y + 3*t^8.94*y | 2*g1^5*t^2.21 + t^2.27/g1^3 + t^2.33/g1^11 + g1^4*t^2.97 + t^3.03/g1^4 + (2*t^3.09)/g1^12 + 2*g1^3*t^3.73 + g1^18*t^4.36 + 4*g1^10*t^4.42 + 3*g1^2*t^4.48 + (3*t^4.55)/g1^6 + t^4.61/g1^14 + t^4.67/g1^22 + 2*g1^9*t^5.18 + 3*g1*t^5.24 + (5*t^5.3)/g1^7 + (2*t^5.36)/g1^15 + (2*t^5.43)/g1^23 + 3*g1^8*t^5.94 - t^6. + (2*t^6.06)/g1^8 + (2*t^6.12)/g1^16 + (3*t^6.18)/g1^24 + 2*g1^23*t^6.57 + 5*g1^15*t^6.64 + 5*g1^7*t^6.7 + (5*t^6.76)/g1 + (5*t^6.82)/g1^9 + (2*t^6.88)/g1^17 + t^6.94/g1^25 + t^7./g1^33 + 3*g1^14*t^7.39 + 6*g1^6*t^7.45 + (7*t^7.52)/g1^2 + (5*t^7.58)/g1^10 + (6*t^7.64)/g1^18 + (2*t^7.7)/g1^26 + (2*t^7.76)/g1^34 + g1^21*t^8.09 + 2*g1^13*t^8.15 - 4*g1^5*t^8.21 + t^8.27/g1^3 + t^8.33/g1^11 + (7*t^8.39)/g1^19 + (3*t^8.46)/g1^27 + (3*t^8.52)/g1^35 + g1^36*t^8.73 + 4*g1^28*t^8.79 + 7*g1^20*t^8.85 + 6*g1^12*t^8.91 + 3*g1^4*t^8.97 - t^4.52/(g1^2*y) - (g1^3*t^6.73)/y - t^6.85/(g1^13*y) + (2*g1^10*t^7.42)/y + (2*g1^2*t^7.48)/y + (2*t^7.55)/(g1^6*y) + (3*g1^9*t^8.18)/y + (3*g1*t^8.24)/y + (7*t^8.3)/(g1^7*y) + (3*t^8.36)/(g1^15*y) + (2*t^8.43)/(g1^23*y) + (3*g1^8*t^8.94)/y - (t^4.52*y)/g1^2 - g1^3*t^6.73*y - (t^6.85*y)/g1^13 + 2*g1^10*t^7.42*y + 2*g1^2*t^7.48*y + (2*t^7.55*y)/g1^6 + 3*g1^9*t^8.18*y + 3*g1*t^8.24*y + (7*t^8.3*y)/g1^7 + (3*t^8.36*y)/g1^15 + (2*t^8.43*y)/g1^23 + 3*g1^8*t^8.94*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46257 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ | 0.6298 | 0.8204 | 0.7677 | [X:[], M:[0.9757, 0.7196, 0.8168], q:[0.7439, 0.2804], qb:[0.4879, 0.4393], phi:[0.5121]] | 2*t^2.16 + t^2.3 + t^2.45 + t^2.78 + t^2.93 + t^3.07 + t^3.22 + 2*t^3.7 + t^4.17 + 4*t^4.32 + 3*t^4.46 + 3*t^4.61 + t^4.76 + t^4.9 + 2*t^4.94 + 3*t^5.09 + 4*t^5.23 + 3*t^5.38 + t^5.52 + t^5.56 + t^5.67 + t^5.71 + 4*t^5.85 - t^4.54/y - t^4.54*y | detail |