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 |
|---|---|---|---|---|---|---|---|---|---|
| 1823 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ | 0.5522 | 0.713 | 0.7744 | [M:[0.8536, 1.0488, 1.1464, 0.756], q:[0.6646, 0.4818], qb:[0.189, 0.7622], phi:[0.4756]] | [M:[[-12], [4], [12], [-20]], q:[[-7], [19]], qb:[[-5], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }M_{4}$, ${ }M_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{3}$, ${ }M_{1}M_{4}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}^{4}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | ${}M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}^{3}$ | 1 | t^2.012 + t^2.268 + 2*t^2.561 + t^2.854 + t^3.146 + 2*t^3.439 + t^3.988 + t^4.025 + 2*t^4.28 + t^4.318 + t^4.536 + t^4.573 + 2*t^4.829 + 2*t^4.866 + 3*t^5.122 + t^5.159 + 4*t^5.414 + t^5.452 + 3*t^5.707 + t^6. + t^6.037 + t^6.256 + 2*t^6.293 + t^6.33 + 2*t^6.548 + 2*t^6.586 + t^6.804 + 2*t^6.841 + 3*t^6.878 + 2*t^7.097 + 2*t^7.134 + t^7.171 + 3*t^7.39 + 2*t^7.427 + t^7.464 + 6*t^7.682 + t^7.72 + 2*t^7.757 + 6*t^7.975 - t^8.012 + t^8.05 + 2*t^8.268 + 2*t^8.305 + t^8.343 + t^8.524 + t^8.598 + t^8.635 + 2*t^8.816 + t^8.891 - t^4.427/y - t^6.695/y + t^7.28/y + (2*t^7.573)/y + (2*t^7.829)/y + t^7.866/y + (2*t^8.122)/y + (2*t^8.159)/y + (3*t^8.414)/y + (2*t^8.452)/y + (4*t^8.707)/y - t^8.963/y - t^4.427*y - t^6.695*y + t^7.28*y + 2*t^7.573*y + 2*t^7.829*y + t^7.866*y + 2*t^8.122*y + 2*t^8.159*y + 3*t^8.414*y + 2*t^8.452*y + 4*t^8.707*y - t^8.963*y | g1^14*t^2.012 + t^2.268/g1^20 + (2*t^2.561)/g1^12 + t^2.854/g1^4 + g1^4*t^3.146 + 2*g1^12*t^3.439 + t^3.988/g1^14 + g1^28*t^4.025 + (2*t^4.28)/g1^6 + g1^36*t^4.318 + t^4.536/g1^40 + g1^2*t^4.573 + (2*t^4.829)/g1^32 + 2*g1^10*t^4.866 + (3*t^5.122)/g1^24 + g1^18*t^5.159 + (4*t^5.414)/g1^16 + g1^26*t^5.452 + (3*t^5.707)/g1^8 + t^6. + g1^42*t^6.037 + t^6.256/g1^34 + 2*g1^8*t^6.293 + g1^50*t^6.33 + (2*t^6.548)/g1^26 + 2*g1^16*t^6.586 + t^6.804/g1^60 + (2*t^6.841)/g1^18 + 3*g1^24*t^6.878 + (2*t^7.097)/g1^52 + (2*t^7.134)/g1^10 + g1^32*t^7.171 + (3*t^7.39)/g1^44 + (2*t^7.427)/g1^2 + g1^40*t^7.464 + (6*t^7.682)/g1^36 + g1^6*t^7.72 + 2*g1^48*t^7.757 + (6*t^7.975)/g1^28 - g1^14*t^8.012 + g1^56*t^8.05 + (2*t^8.268)/g1^20 + 2*g1^22*t^8.305 + g1^64*t^8.343 + t^8.524/g1^54 + g1^30*t^8.598 + g1^72*t^8.635 + (2*t^8.816)/g1^46 + g1^38*t^8.891 - t^4.427/(g1^2*y) - t^6.695/(g1^22*y) + t^7.28/(g1^6*y) + (2*g1^2*t^7.573)/y + (2*t^7.829)/(g1^32*y) + (g1^10*t^7.866)/y + (2*t^8.122)/(g1^24*y) + (2*g1^18*t^8.159)/y + (3*t^8.414)/(g1^16*y) + (2*g1^26*t^8.452)/y + (4*t^8.707)/(g1^8*y) - t^8.963/(g1^42*y) - (t^4.427*y)/g1^2 - (t^6.695*y)/g1^22 + (t^7.28*y)/g1^6 + 2*g1^2*t^7.573*y + (2*t^7.829*y)/g1^32 + g1^10*t^7.866*y + (2*t^8.122*y)/g1^24 + 2*g1^18*t^8.159*y + (3*t^8.414*y)/g1^16 + 2*g1^26*t^8.452*y + (4*t^8.707*y)/g1^8 - (t^8.963*y)/g1^42 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 366 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ | 0.6975 | 0.8554 | 0.8154 | [M:[0.9458, 1.0181, 1.0542, 0.9096], q:[0.4896, 0.5646], qb:[0.4562, 0.5258], phi:[0.491]] | t^2.729 + t^2.837 + t^2.946 + t^3.046 + t^3.054 + t^3.062 + t^3.163 + t^4.21 + t^4.31 + t^4.411 + t^4.419 + t^4.519 + t^4.535 + t^4.628 + t^4.636 + t^4.744 + t^4.86 + t^5.458 + t^5.566 + t^5.675 + 2*t^5.783 + 2*t^5.892 + t^5.992 - 2*t^6. - t^4.473/y - t^4.473*y | detail |