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 |
|---|---|---|---|---|---|---|---|---|---|
| 55899 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ | 0.6751 | 0.8573 | 0.7874 | [M:[1.1368, 0.7052, 0.8632, 0.8105, 0.7052, 0.7578], q:[0.4053, 0.458], qb:[0.8896, 0.7315], phi:[0.3789]] | [M:[[12], [18], [-12], [-2], [18], [8]], q:[[-1], [-11]], qb:[[-17], [13]], phi:[[4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{6}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{2}$ | ${}$ | -1 | 2*t^2.115 + 2*t^2.274 + t^2.432 + t^2.59 + t^3.41 + t^3.568 + t^4.043 + 3*t^4.231 + 4*t^4.389 + 5*t^4.547 + 4*t^4.705 + 4*t^4.863 + t^5.021 + t^5.179 + 2*t^5.526 + 3*t^5.684 + t^5.842 - t^6. + t^6.158 + t^6.316 + 4*t^6.346 + t^6.474 + 6*t^6.504 + t^6.632 + 9*t^6.663 + 11*t^6.821 + 10*t^6.979 + 7*t^7.137 + 2*t^7.295 + t^7.453 + 3*t^7.641 + 5*t^7.799 + 3*t^7.957 + t^8.085 - 2*t^8.115 - 2*t^8.274 - 4*t^8.432 + 5*t^8.462 - 2*t^8.59 + 8*t^8.62 + 13*t^8.778 + 2*t^8.906 + 18*t^8.936 - t^4.137/y - (2*t^6.252)/y - (2*t^6.41)/y - t^6.568/y + t^7.231/y + (4*t^7.389)/y + (3*t^7.547)/y + (5*t^7.705)/y + (4*t^7.863)/y + (3*t^8.021)/y - (3*t^8.368)/y - (2*t^8.526)/y - t^8.684/y + t^8.842/y - t^4.137*y - 2*t^6.252*y - 2*t^6.41*y - t^6.568*y + t^7.231*y + 4*t^7.389*y + 3*t^7.547*y + 5*t^7.705*y + 4*t^7.863*y + 3*t^8.021*y - 3*t^8.368*y - 2*t^8.526*y - t^8.684*y + t^8.842*y | 2*g1^18*t^2.115 + 2*g1^8*t^2.274 + t^2.432/g1^2 + t^2.59/g1^12 + g1^12*t^3.41 + g1^2*t^3.568 + t^4.043/g1^28 + 3*g1^36*t^4.231 + 4*g1^26*t^4.389 + 5*g1^16*t^4.547 + 4*g1^6*t^4.705 + (4*t^4.863)/g1^4 + t^5.021/g1^14 + t^5.179/g1^24 + 2*g1^30*t^5.526 + 3*g1^20*t^5.684 + g1^10*t^5.842 - t^6. + t^6.158/g1^10 + t^6.316/g1^20 + 4*g1^54*t^6.346 + t^6.474/g1^30 + 6*g1^44*t^6.504 + t^6.632/g1^40 + 9*g1^34*t^6.663 + 11*g1^24*t^6.821 + 10*g1^14*t^6.979 + 7*g1^4*t^7.137 + (2*t^7.295)/g1^6 + t^7.453/g1^16 + 3*g1^48*t^7.641 + 5*g1^38*t^7.799 + 3*g1^28*t^7.957 + t^8.085/g1^56 - 2*g1^18*t^8.115 - 2*g1^8*t^8.274 - (4*t^8.432)/g1^2 + 5*g1^72*t^8.462 - (2*t^8.59)/g1^12 + 8*g1^62*t^8.62 + 13*g1^52*t^8.778 + (2*t^8.906)/g1^32 + 18*g1^42*t^8.936 - (g1^4*t^4.137)/y - (2*g1^22*t^6.252)/y - (2*g1^12*t^6.41)/y - (g1^2*t^6.568)/y + (g1^36*t^7.231)/y + (4*g1^26*t^7.389)/y + (3*g1^16*t^7.547)/y + (5*g1^6*t^7.705)/y + (4*t^7.863)/(g1^4*y) + (3*t^8.021)/(g1^14*y) - (3*g1^40*t^8.368)/y - (2*g1^30*t^8.526)/y - (g1^20*t^8.684)/y + (g1^10*t^8.842)/y - g1^4*t^4.137*y - 2*g1^22*t^6.252*y - 2*g1^12*t^6.41*y - g1^2*t^6.568*y + g1^36*t^7.231*y + 4*g1^26*t^7.389*y + 3*g1^16*t^7.547*y + 5*g1^6*t^7.705*y + (4*t^7.863*y)/g1^4 + (3*t^8.021*y)/g1^14 - 3*g1^40*t^8.368*y - 2*g1^30*t^8.526*y - g1^20*t^8.684*y + g1^10*t^8.842*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 |
|---|---|---|---|---|---|---|---|---|---|
| 48141 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ | 0.6565 | 0.8232 | 0.7974 | [M:[1.1417, 0.7126, 0.8583, 0.8097, 0.7126], q:[0.4049, 0.4534], qb:[0.8825, 0.7369], phi:[0.3806]] | 2*t^2.138 + t^2.283 + t^2.429 + t^2.575 + t^3.425 + t^3.571 + t^3.717 + t^4.008 + 3*t^4.276 + 2*t^4.421 + 3*t^4.567 + 3*t^4.713 + 3*t^4.858 + t^5.004 + t^5.15 + 2*t^5.563 + 2*t^5.709 + 2*t^5.854 - t^4.142/y - t^4.142*y | detail |