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 |
|---|---|---|---|---|---|---|---|---|---|
| 1447 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{5}M_{6}$ | 0.6937 | 0.8507 | 0.8155 | [M:[1.007, 0.9789, 1.0211, 0.9648, 1.0352, 0.9648], q:[0.5035, 0.4894], qb:[0.4754, 0.5458], phi:[0.4965]] | [M:[[2], [-6], [6], [-10], [10], [-10]], q:[[1], [-3]], qb:[[-7], [13]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}^{4}$ | ${}$ | -2 | 2*t^2.894 + t^2.937 + t^2.979 + t^3.021 + t^3.063 + t^3.148 + t^4.342 + t^4.384 + 2*t^4.426 + t^4.468 + t^4.511 + t^4.553 + t^4.595 + t^4.637 + t^4.764 + 2*t^5.789 + t^5.831 + 2*t^5.873 + 2*t^5.915 + 2*t^5.958 - 2*t^6. + t^6.042 + t^6.085 + t^6.127 + t^6.296 + 2*t^7.236 + 2*t^7.278 + 4*t^7.32 + 3*t^7.363 + 4*t^7.405 + 2*t^7.447 + 2*t^7.489 + t^7.532 + 2*t^7.574 + t^7.616 + 2*t^7.658 + t^7.701 + t^7.743 + t^7.785 + t^7.827 + t^7.912 + 3*t^8.683 + 2*t^8.725 + 4*t^8.768 + 3*t^8.81 + 4*t^8.852 - 2*t^8.894 - t^8.979 - t^4.489/y - t^7.384/y + t^7.595/y + t^8.789/y + (2*t^8.831)/y + (2*t^8.873)/y + (3*t^8.915)/y + (3*t^8.958)/y - t^4.489*y - t^7.384*y + t^7.595*y + t^8.789*y + 2*t^8.831*y + 2*t^8.873*y + 3*t^8.915*y + 3*t^8.958*y | (2*t^2.894)/g1^10 + t^2.937/g1^6 + t^2.979/g1^2 + g1^2*t^3.021 + g1^6*t^3.063 + g1^14*t^3.148 + t^4.342/g1^15 + t^4.384/g1^11 + (2*t^4.426)/g1^7 + t^4.468/g1^3 + g1*t^4.511 + g1^5*t^4.553 + g1^9*t^4.595 + g1^13*t^4.637 + g1^25*t^4.764 + (2*t^5.789)/g1^20 + t^5.831/g1^16 + (2*t^5.873)/g1^12 + (2*t^5.915)/g1^8 + (2*t^5.958)/g1^4 - 2*t^6. + g1^4*t^6.042 + g1^8*t^6.085 + g1^12*t^6.127 + g1^28*t^6.296 + (2*t^7.236)/g1^25 + (2*t^7.278)/g1^21 + (4*t^7.32)/g1^17 + (3*t^7.363)/g1^13 + (4*t^7.405)/g1^9 + (2*t^7.447)/g1^5 + (2*t^7.489)/g1 + g1^3*t^7.532 + 2*g1^7*t^7.574 + g1^11*t^7.616 + 2*g1^15*t^7.658 + g1^19*t^7.701 + g1^23*t^7.743 + g1^27*t^7.785 + g1^31*t^7.827 + g1^39*t^7.912 + (3*t^8.683)/g1^30 + (2*t^8.725)/g1^26 + (4*t^8.768)/g1^22 + (3*t^8.81)/g1^18 + (4*t^8.852)/g1^14 - (2*t^8.894)/g1^10 - t^8.979/g1^2 - t^4.489/(g1*y) - t^7.384/(g1^11*y) + (g1^9*t^7.595)/y + t^8.789/(g1^20*y) + (2*t^8.831)/(g1^16*y) + (2*t^8.873)/(g1^12*y) + (3*t^8.915)/(g1^8*y) + (3*t^8.958)/(g1^4*y) - (t^4.489*y)/g1 - (t^7.384*y)/g1^11 + g1^9*t^7.595*y + (t^8.789*y)/g1^20 + (2*t^8.831*y)/g1^16 + (2*t^8.873*y)/g1^12 + (3*t^8.915*y)/g1^8 + (3*t^8.958*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|
| 2530 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{1}M_{7}$ | 0.6944 | 0.852 | 0.8151 | [M:[1.0081, 0.9758, 1.0242, 0.9597, 1.0403, 0.9597, 0.9919], q:[0.504, 0.4879], qb:[0.4718, 0.5524], phi:[0.496]] | 2*t^2.879 + t^2.928 + 2*t^2.976 + t^3.072 + t^3.169 + t^4.319 + t^4.367 + 2*t^4.415 + t^4.464 + t^4.512 + t^4.56 + t^4.609 + t^4.657 + t^4.802 + 2*t^5.758 + t^5.807 + 4*t^5.855 + t^5.903 + 3*t^5.952 - 3*t^6. - t^4.488/y - t^4.488*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 |
|---|---|---|---|---|---|---|---|---|---|
| 938 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ | 0.6916 | 0.8474 | 0.8161 | [M:[1.0021, 0.9938, 1.0062, 0.9896, 1.0104], q:[0.501, 0.4969], qb:[0.4927, 0.5135], phi:[0.499]] | t^2.969 + t^2.981 + t^2.994 + t^3.006 + t^3.019 + t^3.031 + t^3.044 + t^4.453 + t^4.466 + 2*t^4.478 + t^4.491 + t^4.503 + t^4.516 + t^4.528 + t^4.54 + t^4.578 + t^5.963 + t^5.975 + t^5.988 - t^6. - t^4.497/y - t^4.497*y | detail |