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 |
|---|---|---|---|---|---|---|---|---|---|
| 56086 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6475 | 0.8091 | 0.8002 | [M:[1.1899, 0.8101, 0.8101, 0.7764, 0.7764, 0.827, 1.2067], q:[0.3882, 0.4219], qb:[0.8017, 0.8017], phi:[0.3966]] | [M:[[-6], [6], [6], [-14], [-14], [16], [4]], q:[[-7], [13]], qb:[[1], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{5}$, ${ }M_{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{4}\phi_{1}q_{1}q_{2}$, ${ }M_{5}\phi_{1}q_{1}q_{2}$ | ${}M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$ | -1 | 2*t^2.329 + 2*t^2.43 + t^2.481 + t^3.57 + 2*t^3.62 + t^3.721 + 3*t^4.658 + 4*t^4.76 + 3*t^4.81 + 3*t^4.861 + 2*t^4.911 + t^4.962 + t^5.899 + 2*t^5.949 - t^6. + 5*t^6.051 + t^6.101 + 2*t^6.152 + t^6.202 + 4*t^6.988 + 5*t^7.089 + 3*t^7.139 + 4*t^7.19 + 4*t^7.24 + 5*t^7.291 + 4*t^7.342 + 2*t^7.392 + 2*t^7.443 + t^8.228 + 2*t^8.279 - 5*t^8.329 + 4*t^8.38 - 3*t^8.43 + 3*t^8.481 + 3*t^8.531 + 4*t^8.582 + 2*t^8.632 + t^8.683 - t^4.19/y - (2*t^6.519)/y - t^6.62/y - t^6.671/y + t^7.658/y + t^7.709/y + (5*t^7.76)/y + (2*t^7.81)/y + (3*t^7.861)/y + (2*t^7.911)/y - (3*t^8.848)/y + (2*t^8.899)/y + (2*t^8.949)/y - t^4.19*y - 2*t^6.519*y - t^6.62*y - t^6.671*y + t^7.658*y + t^7.709*y + 5*t^7.76*y + 2*t^7.81*y + 3*t^7.861*y + 2*t^7.911*y - 3*t^8.848*y + 2*t^8.899*y + 2*t^8.949*y | (2*t^2.329)/g1^14 + 2*g1^6*t^2.43 + g1^16*t^2.481 + t^3.57/g1^6 + 2*g1^4*t^3.62 + g1^24*t^3.721 + (3*t^4.658)/g1^28 + (4*t^4.76)/g1^8 + 3*g1^2*t^4.81 + 3*g1^12*t^4.861 + 2*g1^22*t^4.911 + g1^32*t^4.962 + t^5.899/g1^20 + (2*t^5.949)/g1^10 - t^6. + 5*g1^10*t^6.051 + g1^20*t^6.101 + 2*g1^30*t^6.152 + g1^40*t^6.202 + (4*t^6.988)/g1^42 + (5*t^7.089)/g1^22 + (3*t^7.139)/g1^12 + (4*t^7.19)/g1^2 + 4*g1^8*t^7.24 + 5*g1^18*t^7.291 + 4*g1^28*t^7.342 + 2*g1^38*t^7.392 + 2*g1^48*t^7.443 + t^8.228/g1^34 + (2*t^8.279)/g1^24 - (5*t^8.329)/g1^14 + (4*t^8.38)/g1^4 - 3*g1^6*t^8.43 + 3*g1^16*t^8.481 + 3*g1^26*t^8.531 + 4*g1^36*t^8.582 + 2*g1^46*t^8.632 + g1^56*t^8.683 - t^4.19/(g1^2*y) - (2*t^6.519)/(g1^16*y) - (g1^4*t^6.62)/y - (g1^14*t^6.671)/y + t^7.658/(g1^28*y) + t^7.709/(g1^18*y) + (5*t^7.76)/(g1^8*y) + (2*g1^2*t^7.81)/y + (3*g1^12*t^7.861)/y + (2*g1^22*t^7.911)/y - (3*t^8.848)/(g1^30*y) + (2*t^8.899)/(g1^20*y) + (2*t^8.949)/(g1^10*y) - (t^4.19*y)/g1^2 - (2*t^6.519*y)/g1^16 - g1^4*t^6.62*y - g1^14*t^6.671*y + (t^7.658*y)/g1^28 + (t^7.709*y)/g1^18 + (5*t^7.76*y)/g1^8 + 2*g1^2*t^7.81*y + 3*g1^12*t^7.861*y + 2*g1^22*t^7.911*y - (3*t^8.848*y)/g1^30 + (2*t^8.899*y)/g1^20 + (2*t^8.949*y)/g1^10 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 50948 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ | 0.6644 | 0.8389 | 0.792 | [M:[1.1879, 0.8121, 0.8121, 0.7717, 0.7717, 0.8324], q:[0.3858, 0.4263], qb:[0.802, 0.802], phi:[0.396]] | 2*t^2.315 + t^2.376 + 2*t^2.436 + t^2.497 + t^3.564 + t^3.624 + t^3.746 + 3*t^4.63 + 2*t^4.691 + 5*t^4.751 + 5*t^4.812 + 4*t^4.873 + 2*t^4.934 + t^4.994 + t^5.879 + t^5.939 - t^4.188/y - t^4.188*y | detail |