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 |
|---|---|---|---|---|---|---|---|---|---|
| 1441 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}M_{6}$ | 0.6914 | 0.848 | 0.8153 | [M:[0.9992, 1.0025, 0.9975, 1.0042, 0.9958, 0.9975], q:[0.4996, 0.5013], qb:[0.503, 0.4945], phi:[0.5004]] | [M:[[2], [-6], [6], [-10], [10], [6]], q:[[1], [-3]], qb:[[-7], [13]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.982 + t^2.987 + 2*t^2.992 + t^2.997 + t^3.003 + t^3.013 + t^4.468 + t^4.484 + t^4.489 + t^4.494 + t^4.499 + t^4.504 + 2*t^4.509 + t^4.514 + t^4.519 + t^5.965 + t^5.97 + 2*t^5.975 + 2*t^5.98 + 4*t^5.985 + 2*t^5.99 + t^5.995 - 2*t^6. + t^6.005 - t^6.02 + t^7.451 + t^7.456 + 2*t^7.461 + t^7.466 + 2*t^7.471 + 2*t^7.476 + 3*t^7.481 + 3*t^7.486 + 3*t^7.491 + 2*t^7.496 + 3*t^7.501 + 2*t^7.506 + 3*t^7.511 + t^7.522 + t^7.532 + t^8.937 + t^8.947 + 2*t^8.952 + 3*t^8.957 + 3*t^8.962 + 4*t^8.967 + 3*t^8.972 + 6*t^8.977 + t^8.982 - 4*t^8.992 - t^8.997 - t^4.501/y - t^7.494/y + t^7.509/y + t^8.97/y + (2*t^8.975)/y + (3*t^8.98)/y + (3*t^8.985)/y + (3*t^8.99)/y + (3*t^8.995)/y - t^4.501*y - t^7.494*y + t^7.509*y + t^8.97*y + 2*t^8.975*y + 3*t^8.98*y + 3*t^8.985*y + 3*t^8.99*y + 3*t^8.995*y | g1^14*t^2.982 + g1^10*t^2.987 + 2*g1^6*t^2.992 + g1^2*t^2.997 + t^3.003/g1^2 + t^3.013/g1^10 + g1^25*t^4.468 + g1^13*t^4.484 + g1^9*t^4.489 + g1^5*t^4.494 + g1*t^4.499 + t^4.504/g1^3 + (2*t^4.509)/g1^7 + t^4.514/g1^11 + t^4.519/g1^15 + g1^28*t^5.965 + g1^24*t^5.97 + 2*g1^20*t^5.975 + 2*g1^16*t^5.98 + 4*g1^12*t^5.985 + 2*g1^8*t^5.99 + g1^4*t^5.995 - 2*t^6. + t^6.005/g1^4 - t^6.02/g1^16 + g1^39*t^7.451 + g1^35*t^7.456 + 2*g1^31*t^7.461 + g1^27*t^7.466 + 2*g1^23*t^7.471 + 2*g1^19*t^7.476 + 3*g1^15*t^7.481 + 3*g1^11*t^7.486 + 3*g1^7*t^7.491 + 2*g1^3*t^7.496 + (3*t^7.501)/g1 + (2*t^7.506)/g1^5 + (3*t^7.511)/g1^9 + t^7.522/g1^17 + t^7.532/g1^25 + g1^50*t^8.937 + g1^42*t^8.947 + 2*g1^38*t^8.952 + 3*g1^34*t^8.957 + 3*g1^30*t^8.962 + 4*g1^26*t^8.967 + 3*g1^22*t^8.972 + 6*g1^18*t^8.977 + g1^14*t^8.982 - 4*g1^6*t^8.992 - g1^2*t^8.997 - t^4.501/(g1*y) - (g1^5*t^7.494)/y + t^7.509/(g1^7*y) + (g1^24*t^8.97)/y + (2*g1^20*t^8.975)/y + (3*g1^16*t^8.98)/y + (3*g1^12*t^8.985)/y + (3*g1^8*t^8.99)/y + (3*g1^4*t^8.995)/y - (t^4.501*y)/g1 - g1^5*t^7.494*y + (t^7.509*y)/g1^7 + g1^24*t^8.97*y + 2*g1^20*t^8.975*y + 3*g1^16*t^8.98*y + 3*g1^12*t^8.985*y + 3*g1^8*t^8.99*y + 3*g1^4*t^8.995*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 |
|---|---|---|---|---|---|---|---|---|---|
| 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 |