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 |
|---|---|---|---|---|---|---|---|---|---|
| 895 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ | 0.7115 | 0.8652 | 0.8224 | [M:[0.993, 0.8397, 1.007, 0.8257, 0.993, 1.1743], q:[0.4582, 0.5488], qb:[0.5348, 0.6254], phi:[0.4582]] | [M:[[1, -1], [-1, -3], [-1, 1], [1, -5], [1, -1], [-1, 5]], q:[[0, -1], [-1, 2]], qb:[[1, 0], [0, 3]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$ | ${}\phi_{1}^{2}q_{1}\tilde{q}_{2}$ | -2 | t^2.519 + t^2.749 + 2*t^2.979 + 2*t^3.251 + t^3.523 + t^4.124 + t^4.354 + t^4.396 + t^4.583 + 2*t^4.625 + t^4.667 + t^4.855 + t^4.897 + t^5.038 + t^5.127 + t^5.268 + 2*t^5.498 + 2*t^5.958 - 2*t^6. + 2*t^6.23 - t^6.272 + 3*t^6.502 + t^6.643 + 2*t^6.774 + t^6.873 + t^6.915 + t^7.046 + 2*t^7.103 + t^7.145 + t^7.187 + 2*t^7.333 + 2*t^7.375 + t^7.417 + t^7.558 + 2*t^7.562 + 2*t^7.604 + 2*t^7.646 + t^7.788 + 2*t^7.834 + 2*t^7.876 + t^7.918 + 2*t^8.017 + 2*t^8.106 + t^8.148 + t^8.19 + 2*t^8.247 + t^8.378 + t^8.42 + 2*t^8.477 - 2*t^8.519 + t^8.65 - t^8.749 + 3*t^8.937 - 6*t^8.979 - t^4.375/y - t^6.894/y - t^7.124/y - t^7.354/y + t^7.396/y + t^7.625/y + t^7.855/y + t^8.268/y + (2*t^8.498)/y + (2*t^8.728)/y + (2*t^8.77)/y + t^8.958/y - t^4.375*y - t^6.894*y - t^7.124*y - t^7.354*y + t^7.396*y + t^7.625*y + t^7.855*y + t^8.268*y + 2*t^8.498*y + 2*t^8.728*y + 2*t^8.77*y + t^8.958*y | t^2.519/(g1*g2^3) + t^2.749/g2^2 + (2*g1*t^2.979)/g2 + 2*g2^2*t^3.251 + (g2^5*t^3.523)/g1 + t^4.124/g2^3 + (g1*t^4.354)/g2^2 + t^4.396/g1 + (g1^2*t^4.583)/g2 + 2*g2*t^4.625 + (g2^3*t^4.667)/g1^2 + g1*g2^2*t^4.855 + (g2^4*t^4.897)/g1 + t^5.038/(g1^2*g2^6) + g2^5*t^5.127 + t^5.268/(g1*g2^5) + (2*t^5.498)/g2^4 + (2*g1^2*t^5.958)/g2^2 - 2*t^6. + 2*g1*g2*t^6.23 - (g2^3*t^6.272)/g1 + 3*g2^4*t^6.502 + t^6.643/(g1*g2^6) + (2*g2^7*t^6.774)/g1 + t^6.873/g2^5 + t^6.915/(g1^2*g2^3) + (g2^10*t^7.046)/g1^2 + (2*g1*t^7.103)/g2^4 + t^7.145/(g1*g2^2) + t^7.187/g1^3 + (2*g1^2*t^7.333)/g2^3 + (2*t^7.375)/g2 + (g2*t^7.417)/g1^2 + t^7.558/(g1^3*g2^9) + (2*g1^3*t^7.562)/g2^2 + 2*g1*t^7.604 + (2*g2^2*t^7.646)/g1 + t^7.788/(g1^2*g2^8) + 2*g1^2*g2*t^7.834 + 2*g2^3*t^7.876 + (g2^5*t^7.918)/g1^2 + (2*t^8.017)/(g1*g2^7) + 2*g1*g2^4*t^8.106 + (g2^6*t^8.148)/g1 + (g2^8*t^8.19)/g1^3 + (2*t^8.247)/g2^6 + g2^7*t^8.378 + (g2^9*t^8.42)/g1^2 + (2*g1*t^8.477)/g2^5 - (2*t^8.519)/(g1*g2^3) + (g2^10*t^8.65)/g1 - t^8.749/g2^2 + (3*g1^3*t^8.937)/g2^3 - (6*g1*t^8.979)/g2 - t^4.375/(g2*y) - t^6.894/(g1*g2^4*y) - t^7.124/(g2^3*y) - (g1*t^7.354)/(g2^2*y) + t^7.396/(g1*y) + (g2*t^7.625)/y + (g1*g2^2*t^7.855)/y + t^8.268/(g1*g2^5*y) + (2*t^8.498)/(g2^4*y) + (2*g1*t^8.728)/(g2^3*y) + (2*t^8.77)/(g1*g2*y) + (g1^2*t^8.958)/(g2^2*y) - (t^4.375*y)/g2 - (t^6.894*y)/(g1*g2^4) - (t^7.124*y)/g2^3 - (g1*t^7.354*y)/g2^2 + (t^7.396*y)/g1 + g2*t^7.625*y + g1*g2^2*t^7.855*y + (t^8.268*y)/(g1*g2^5) + (2*t^8.498*y)/g2^4 + (2*g1*t^8.728*y)/g2^3 + (2*t^8.77*y)/(g1*g2) + (g1^2*t^8.958*y)/g2^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 579 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ | 0.7283 | 0.8957 | 0.8131 | [M:[0.9749, 0.82, 1.0251, 0.7699, 0.9749], q:[0.4487, 0.5763], qb:[0.5262, 0.6538], phi:[0.4487]] | t^2.31 + t^2.46 + t^2.692 + 2*t^2.925 + 2*t^3.308 + t^4.039 + t^4.271 + t^4.421 + t^4.503 + t^4.62 + 2*t^4.654 + t^4.77 + t^4.804 + t^4.886 + t^4.92 + t^5.002 + t^5.036 + t^5.153 + 2*t^5.235 + t^5.269 + 2*t^5.385 + 2*t^5.617 + 2*t^5.85 - 2*t^6. - t^4.346/y - t^4.346*y | detail |