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 |
|---|---|---|---|---|---|---|---|---|---|
| 100 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_2$ | 0.6732 | 0.7929 | 0.8491 | [X:[], M:[0.8614, 1.2464, 0.8614], q:[0.8116, 0.596], qb:[0.5426, 0.5426], phi:[0.3768]] | [X:[], M:[[-7, -7, 0], [4, 4, 4], [-7, 0, -7]], q:[[1, 1, 1], [7, 0, 0]], qb:[[0, 7, 0], [0, 0, 7]], phi:[[-2, -2, -2]]] | 3 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ M_3$, $ \tilde{q}_1\tilde{q}_2$, $ M_2$, $ q_1\tilde{q}_1$, $ q_1\tilde{q}_2$, $ q_1q_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ M_1^2$, $ M_3^2$, $ M_1M_3$ | . | -5 | 2*t^2.58 + t^3.26 + t^3.74 + 2*t^4.06 + t^4.22 + 3*t^4.39 + 2*t^4.55 + t^4.71 + 3*t^5.17 - 5*t^6. - 2*t^6.16 - t^6.48 + t^6.51 + 3*t^6.65 + 4*t^6.97 + t^6.99 + 2*t^7.32 + t^7.48 + 3*t^7.64 + 4*t^7.75 + 2*t^7.8 + t^7.96 + 3*t^8.13 + 2*t^8.29 + 5*t^8.45 - 8*t^8.58 + 3*t^8.61 - t^8.74 + 7*t^8.77 + 3*t^8.93 - t^4.13/y - (2*t^6.71)/y + (2*t^7.55)/y + t^8.17/y + (2*t^8.84)/y - t^4.13*y - 2*t^6.71*y + 2*t^7.55*y + t^8.17*y + 2*t^8.84*y | t^2.58/(g1^7*g2^7) + t^2.58/(g1^7*g3^7) + g2^7*g3^7*t^3.26 + g1^4*g2^4*g3^4*t^3.74 + g1*g2^8*g3*t^4.06 + g1*g2*g3^8*t^4.06 + g1^8*g2*g3*t^4.22 + (g2^12*t^4.39)/(g1^2*g3^2) + (g2^5*g3^5*t^4.39)/g1^2 + (g3^12*t^4.39)/(g1^2*g2^2) + (g1^5*g2^5*t^4.55)/g3^2 + (g1^5*g3^5*t^4.55)/g2^2 + (g1^12*t^4.71)/(g2^2*g3^2) + t^5.17/(g1^14*g2^14) + t^5.17/(g1^14*g3^14) + t^5.17/(g1^14*g2^7*g3^7) - 3*t^6. - (g2^7*t^6.)/g3^7 - (g3^7*t^6.)/g2^7 - (g1^7*t^6.16)/g2^7 - (g1^7*t^6.16)/g3^7 - (g1^4*t^6.48)/(g2^3*g3^3) + g2^14*g3^14*t^6.51 + (g2^8*t^6.65)/(g1^6*g3^6) + (g2*g3*t^6.65)/g1^6 + (g3^8*t^6.65)/(g1^6*g2^6) + (g2^12*t^6.97)/(g1^9*g3^9) + (g2^5*t^6.97)/(g1^9*g3^2) + (g3^5*t^6.97)/(g1^9*g2^2) + (g3^12*t^6.97)/(g1^9*g2^9) + g1^4*g2^11*g3^11*t^6.99 + g1*g2^15*g3^8*t^7.32 + g1*g2^8*g3^15*t^7.32 + g1^8*g2^8*g3^8*t^7.48 + (g2^19*g3^5*t^7.64)/g1^2 + (g2^12*g3^12*t^7.64)/g1^2 + (g2^5*g3^19*t^7.64)/g1^2 + t^7.75/(g1^21*g2^21) + t^7.75/(g1^21*g3^21) + t^7.75/(g1^21*g2^7*g3^14) + t^7.75/(g1^21*g2^14*g3^7) + g1^5*g2^12*g3^5*t^7.8 + g1^5*g2^5*g3^12*t^7.8 + g1^12*g2^5*g3^5*t^7.96 + g1^2*g2^16*g3^2*t^8.13 + g1^2*g2^9*g3^9*t^8.13 + g1^2*g2^2*g3^16*t^8.13 + g1^9*g2^9*g3^2*t^8.29 + g1^9*g2^2*g3^9*t^8.29 + (g2^20*t^8.45)/(g1*g3) + g1^16*g2^2*g3^2*t^8.45 + (g2^13*g3^6*t^8.45)/g1 + (g2^6*g3^13*t^8.45)/g1 + (g3^20*t^8.45)/(g1*g2) - (3*t^8.58)/(g1^7*g2^7) - (g2^7*t^8.58)/(g1^7*g3^14) - (3*t^8.58)/(g1^7*g3^7) - (g3^7*t^8.58)/(g1^7*g2^14) + (g1^6*g2^13*t^8.61)/g3 + g1^6*g2^6*g3^6*t^8.61 + (g1^6*g3^13*t^8.61)/g2 - t^8.74/(g2^7*g3^7) + (g2^24*t^8.77)/(g1^4*g3^4) + (g1^13*g2^6*t^8.77)/g3 + (g2^17*g3^3*t^8.77)/g1^4 + (g1^13*g3^6*t^8.77)/g2 + (g2^10*g3^10*t^8.77)/g1^4 + (g2^3*g3^17*t^8.77)/g1^4 + (g3^24*t^8.77)/(g1^4*g2^4) + (g1^3*g2^17*t^8.93)/g3^4 + (g1^20*t^8.93)/(g2*g3) + (g1^3*g3^17*t^8.93)/g2^4 - t^4.13/(g1^2*g2^2*g3^2*y) - t^6.71/(g1^9*g2^2*g3^9*y) - t^6.71/(g1^9*g2^9*g3^2*y) + (g1^5*g2^5*t^7.55)/(g3^2*y) + (g1^5*g3^5*t^7.55)/(g2^2*y) + t^8.17/(g1^14*g2^7*g3^7*y) + (g2^7*t^8.84)/(g1^7*y) + (g3^7*t^8.84)/(g1^7*y) - (t^4.13*y)/(g1^2*g2^2*g3^2) - (t^6.71*y)/(g1^9*g2^2*g3^9) - (t^6.71*y)/(g1^9*g2^9*g3^2) + (g1^5*g2^5*t^7.55*y)/g3^2 + (g1^5*g3^5*t^7.55*y)/g2^2 + (t^8.17*y)/(g1^14*g2^7*g3^7) + (g2^7*t^8.84*y)/g1^7 + (g3^7*t^8.84*y)/g1^7 |
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 |
|---|---|---|---|---|---|---|---|---|
| 159 | $\phi_1q_1^2$ + $ 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$ | 0.6845 | 0.8095 | 0.8456 | [X:[], M:[0.8373, 1.2823, 0.8373, 0.8373], q:[0.8206, 0.5813], qb:[0.5813, 0.5813], phi:[0.3588]] | 3*t^2.51 + t^3.85 + 3*t^4.21 + 6*t^4.56 + 6*t^5.02 - 9*t^6. - t^4.08/y - t^4.08*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 65 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ | 0.6643 | 0.7825 | 0.849 | [X:[], M:[0.8927, 1.2048], q:[0.8012, 0.5537], qb:[0.5537, 0.501], phi:[0.3976]] | t^2.68 + 2*t^3.16 + t^3.61 + t^3.91 + 2*t^4.06 + t^4.2 + 2*t^4.36 + 3*t^4.51 + t^5.36 - 5*t^6. - t^4.19/y - t^4.19*y | detail |