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 |
|---|---|---|---|---|---|---|---|---|---|
| 963 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}M_{6}$ | 0.7092 | 0.8704 | 0.8148 | [M:[0.8407, 1.0531, 0.8964, 0.9975, 1.0025, 0.9975], q:[0.6327, 0.5265], qb:[0.4709, 0.476], phi:[0.4735]] | [M:[[6, 6], [-2, -2], [3, 5], [1, -1], [-1, 1], [1, -1]], q:[[-5, -5], [-1, -1]], qb:[[2, 0], [0, 2]], phi:[[1, 1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{6}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$ | ${}$ | -3 | t^2.522 + t^2.689 + t^2.841 + 2*t^2.992 + t^3.159 + t^3.326 + t^4.246 + t^4.261 + t^4.276 + t^4.413 + t^4.428 + t^4.58 + t^4.731 + t^4.747 + t^4.898 + t^5.044 + t^5.211 + t^5.217 + t^5.363 + t^5.378 + t^5.514 + 3*t^5.681 + t^5.833 + t^5.848 + 2*t^5.985 - 3*t^6. + t^6.152 + t^6.319 - t^6.47 + t^6.652 + t^6.768 + t^6.783 + t^6.798 + t^6.935 + t^6.95 + t^6.965 + t^7.086 + 2*t^7.102 + 2*t^7.117 + 2*t^7.238 + 2*t^7.253 + 3*t^7.269 + t^7.405 + t^7.42 + t^7.566 + 2*t^7.572 + t^7.587 + t^7.603 + t^7.724 + t^7.733 + t^7.739 + t^7.885 + t^7.9 + t^8.037 + t^8.058 + t^8.067 + t^8.073 + 3*t^8.204 + t^8.209 + 2*t^8.37 + t^8.492 + t^8.507 - t^8.522 + t^8.537 + t^8.543 + t^8.553 + t^8.658 + 3*t^8.674 - 3*t^8.689 + t^8.704 + t^8.825 - 2*t^8.841 - t^8.856 + 3*t^8.977 - 5*t^8.992 - t^4.42/y - t^6.942/y - t^7.109/y - t^7.413/y + t^7.428/y + t^7.731/y + t^7.898/y + t^8.211/y + t^8.363/y + (2*t^8.514)/y + t^8.53/y + (3*t^8.681)/y + (2*t^8.833)/y + (2*t^8.848)/y + t^8.985/y - t^4.42*y - t^6.942*y - t^7.109*y - t^7.413*y + t^7.428*y + t^7.731*y + t^7.898*y + t^8.211*y + t^8.363*y + 2*t^8.514*y + t^8.53*y + 3*t^8.681*y + 2*t^8.833*y + 2*t^8.848*y + t^8.985*y | g1^6*g2^6*t^2.522 + g1^3*g2^5*t^2.689 + g1^2*g2^2*t^2.841 + (2*g1*t^2.992)/g2 + t^3.159/(g1^2*g2^2) + t^3.326/(g1^5*g2^3) + g1^5*g2*t^4.246 + g1^3*g2^3*t^4.261 + g1*g2^5*t^4.276 + g1^2*t^4.413 + g2^2*t^4.428 + t^4.58/(g1*g2) + t^4.731/(g1^2*g2^4) + t^4.747/(g1^4*g2^2) + t^4.898/(g1^5*g2^5) + g1^12*g2^12*t^5.044 + g1^9*g2^11*t^5.211 + t^5.217/(g1^9*g2^9) + g1^8*g2^8*t^5.363 + g1^6*g2^10*t^5.378 + g1^7*g2^5*t^5.514 + 3*g1^4*g2^4*t^5.681 + g1^3*g2*t^5.833 + g1*g2^3*t^5.848 + (2*g1^2*t^5.985)/g2^2 - 3*t^6. + t^6.152/(g1*g2^3) + t^6.319/(g1^4*g2^4) - t^6.47/(g1^5*g2^7) + t^6.652/(g1^10*g2^6) + g1^11*g2^7*t^6.768 + g1^9*g2^9*t^6.783 + g1^7*g2^11*t^6.798 + g1^8*g2^6*t^6.935 + g1^6*g2^8*t^6.95 + g1^4*g2^10*t^6.965 + g1^7*g2^3*t^7.086 + 2*g1^5*g2^5*t^7.102 + 2*g1^3*g2^7*t^7.117 + 2*g1^6*t^7.238 + 2*g1^4*g2^2*t^7.253 + 3*g1^2*g2^4*t^7.269 + (g1^3*t^7.405)/g2 + g1*g2*t^7.42 + g1^18*g2^18*t^7.566 + (2*t^7.572)/g2^2 + t^7.587/g1^2 + (g2^2*t^7.603)/g1^4 + t^7.724/(g1*g2^5) + g1^15*g2^17*t^7.733 + t^7.739/(g1^3*g2^3) + g1^14*g2^14*t^7.885 + g1^12*g2^16*t^7.9 + g1^13*g2^11*t^8.037 + t^8.058/(g1^7*g2^7) + g1^9*g2^15*t^8.067 + t^8.073/(g1^9*g2^5) + 3*g1^10*g2^10*t^8.204 + t^8.209/(g1^8*g2^10) + 2*g1^7*g2^9*t^8.37 + g1^10*g2^2*t^8.492 + g1^8*g2^4*t^8.507 - g1^6*g2^6*t^8.522 + g1^4*g2^8*t^8.537 + t^8.543/(g1^14*g2^12) + g1^2*g2^10*t^8.553 + g1^7*g2*t^8.658 + 3*g1^5*g2^3*t^8.674 - 3*g1^3*g2^5*t^8.689 + g1*g2^7*t^8.704 + g1^4*t^8.825 - 2*g1^2*g2^2*t^8.841 - g2^4*t^8.856 + (3*g1^3*t^8.977)/g2^3 - (5*g1*t^8.992)/g2 - (g1*g2*t^4.42)/y - (g1^7*g2^7*t^6.942)/y - (g1^4*g2^6*t^7.109)/y - (g1^2*t^7.413)/y + (g2^2*t^7.428)/y + t^7.731/(g1^2*g2^4*y) + t^7.898/(g1^5*g2^5*y) + (g1^9*g2^11*t^8.211)/y + (g1^8*g2^8*t^8.363)/y + (2*g1^7*g2^5*t^8.514)/y + (g1^5*g2^7*t^8.53)/y + (3*g1^4*g2^4*t^8.681)/y + (2*g1^3*g2*t^8.833)/y + (2*g1*g2^3*t^8.848)/y + (g1^2*t^8.985)/(g2^2*y) - g1*g2*t^4.42*y - g1^7*g2^7*t^6.942*y - g1^4*g2^6*t^7.109*y - g1^2*t^7.413*y + g2^2*t^7.428*y + (t^7.731*y)/(g1^2*g2^4) + (t^7.898*y)/(g1^5*g2^5) + g1^9*g2^11*t^8.211*y + g1^8*g2^8*t^8.363*y + 2*g1^7*g2^5*t^8.514*y + g1^5*g2^7*t^8.53*y + 3*g1^4*g2^4*t^8.681*y + 2*g1^3*g2*t^8.833*y + 2*g1*g2^3*t^8.848*y + (g1^2*t^8.985*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 |
|---|---|---|---|---|---|---|---|---|---|
| 600 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ | 0.7101 | 0.8727 | 0.8137 | [M:[0.8432, 1.0523, 0.8729, 1.0226, 0.9774], q:[0.6307, 0.5261], qb:[0.4964, 0.4513], phi:[0.4739]] | t^2.53 + t^2.619 + t^2.843 + t^2.932 + t^3.068 + t^3.157 + t^3.246 + t^4.129 + t^4.265 + t^4.354 + t^4.4 + t^4.489 + t^4.578 + t^4.668 + t^4.803 + t^4.892 + t^5.059 + t^5.148 + t^5.206 + t^5.237 + t^5.373 + t^5.462 + t^5.551 + 2*t^5.686 + 2*t^5.776 + t^5.865 - 2*t^6. - t^4.422/y - t^4.422*y | detail |