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 |
|---|---|---|---|---|---|---|---|---|---|
| 1036 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_4^2$ + $ M_5q_1\tilde{q}_1$ + $ M_1^2$ + $ M_3M_6$ | 0.6784 | 0.8213 | 0.826 | [X:[], M:[1.0, 1.1426, 1.0008, 1.0, 0.714, 0.9992], q:[0.7857, 0.4996], qb:[0.5004, 0.4996], phi:[0.4287]] | [X:[], M:[[0], [4], [-14], [0], [6], [14]], q:[[1], [7]], qb:[[-7], [7]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ M_1$, $ M_4$, $ M_6$, $ M_6$, $ M_2$, $ q_1q_2$, $ q_1\tilde{q}_2$, $ M_5^2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1M_5$, $ M_4M_5$, $ M_5M_6$, $ M_2M_5$ | $M_1M_4$, $ M_1M_6$, $ M_4M_6$, $ M_6^2$, $ M_5q_1q_2$, $ M_5q_1\tilde{q}_2$ | -1 | t^2.14 + 3*t^3. + t^3.43 + 2*t^3.86 + 4*t^4.28 + 3*t^4.29 + 3*t^5.14 + t^5.57 - t^6. + 7*t^6.43 + 2*t^6.85 + t^6.86 + 12*t^7.28 + 4*t^7.71 + 3*t^8.14 + 18*t^8.57 + t^8.58 + t^8.99 - t^4.29/y - t^6.43/y + (4*t^8.14)/y - t^4.29*y - t^6.43*y + 4*t^8.14*y | g1^6*t^2.14 + 2*t^3. + g1^14*t^3. + g1^4*t^3.43 + 2*g1^8*t^3.86 + 4*g1^12*t^4.28 + t^4.29/g1^16 + (2*t^4.29)/g1^2 + 2*g1^6*t^5.14 + g1^20*t^5.14 + g1^10*t^5.57 - 2*t^6. - (2*t^6.)/g1^14 + 2*g1^14*t^6. + g1^28*t^6. + 2*g1^4*t^6.43 + 5*g1^18*t^6.43 + 2*g1^22*t^6.85 - (2*t^6.86)/g1^6 + 3*g1^8*t^6.86 + 8*g1^12*t^7.28 + 4*g1^26*t^7.28 + 4*g1^16*t^7.71 - (2*t^8.14)/g1^8 - 2*g1^6*t^8.14 + 6*g1^20*t^8.14 + g1^34*t^8.14 + (2*t^8.57)/g1^18 + (2*t^8.57)/g1^4 + 4*g1^10*t^8.57 + 10*g1^24*t^8.57 + t^8.58/g1^32 + g1^42*t^8.99 - t^4.29/(g1^2*y) - (g1^4*t^6.43)/y + t^8.14/(g1^8*y) + (2*g1^6*t^8.14)/y + (g1^20*t^8.14)/y - (t^4.29*y)/g1^2 - g1^4*t^6.43*y + (t^8.14*y)/g1^8 + 2*g1^6*t^8.14*y + g1^20*t^8.14*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 |
|---|---|---|---|---|---|---|---|---|---|
| 650 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_4^2$ + $ M_5q_1\tilde{q}_1$ + $ M_1^2$ | 0.6814 | 0.8225 | 0.8284 | [X:[], M:[1.0, 1.1613, 0.9353, 1.0, 0.742], q:[0.7903, 0.5323], qb:[0.4677, 0.5323], phi:[0.4193]] | t^2.23 + t^2.81 + 2*t^3. + t^3.48 + 2*t^3.97 + t^4.06 + 2*t^4.26 + 4*t^4.45 + t^5.03 + 2*t^5.23 + t^5.61 + t^5.71 - 2*t^6. - t^4.26/y - t^4.26*y | detail |