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 |
|---|---|---|---|---|---|---|---|---|---|
| 2868 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{3}M_{6}$ | 0.6513 | 0.8048 | 0.8093 | [M:[1.1559, 1.0887, 0.9449, 0.8441, 0.7339, 1.0551], q:[0.7722, 0.3501], qb:[0.494, 0.5612], phi:[0.4556]] | [M:[[8], [-4], [10], [-8], [12], [-10]], q:[[-1], [3]], qb:[[-11], [1]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}q_{1}q_{2}$ | ${}$ | -1 | t^2.202 + t^2.532 + t^2.734 + t^3.165 + t^3.266 + t^3.367 + t^3.468 + t^3.899 + t^4. + t^4.101 + t^4.331 + t^4.403 + t^4.532 + 2*t^4.734 + t^4.935 + t^5.065 + t^5.266 + 2*t^5.468 + t^5.669 + t^5.698 + 2*t^5.899 - t^6. + t^6.101 + t^6.202 + t^6.302 + t^6.331 + t^6.431 + 2*t^6.532 + t^6.605 + t^6.633 + t^6.734 + t^6.835 + t^6.863 + 2*t^6.935 + 2*t^7.065 + t^7.137 + 3*t^7.266 + 3*t^7.468 + t^7.496 + t^7.597 + 2*t^7.669 + t^7.698 + t^7.798 + t^7.871 + t^7.899 + t^8. + t^8.101 + t^8.202 + 2*t^8.23 + t^8.403 + 2*t^8.431 + t^8.504 - 2*t^8.532 + 2*t^8.633 + t^8.661 - t^8.734 + t^8.806 + t^8.835 + 2*t^8.863 - t^4.367/y - t^6.569/y + t^7.734/y + t^7.935/y + t^8.165/y + t^8.266/y + t^8.367/y + t^8.468/y + t^8.569/y + t^8.669/y + t^8.698/y - t^8.77/y + t^8.798/y + (2*t^8.899)/y - t^4.367*y - t^6.569*y + t^7.734*y + t^7.935*y + t^8.165*y + t^8.266*y + t^8.367*y + t^8.468*y + t^8.569*y + t^8.669*y + t^8.698*y - t^8.77*y + t^8.798*y + 2*t^8.899*y | g1^12*t^2.202 + t^2.532/g1^8 + g1^4*t^2.734 + t^3.165/g1^10 + t^3.266/g1^4 + g1^2*t^3.367 + g1^8*t^3.468 + t^3.899/g1^6 + t^4. + g1^6*t^4.101 + t^4.331/g1^20 + g1^24*t^4.403 + t^4.532/g1^8 + 2*g1^4*t^4.734 + g1^16*t^4.935 + t^5.065/g1^16 + t^5.266/g1^4 + 2*g1^8*t^5.468 + g1^20*t^5.669 + t^5.698/g1^18 + (2*t^5.899)/g1^6 - t^6. + g1^6*t^6.101 + g1^12*t^6.202 + g1^18*t^6.302 + t^6.331/g1^20 + t^6.431/g1^14 + (2*t^6.532)/g1^8 + g1^36*t^6.605 + t^6.633/g1^2 + g1^4*t^6.734 + g1^10*t^6.835 + t^6.863/g1^28 + 2*g1^16*t^6.935 + (2*t^7.065)/g1^16 + g1^28*t^7.137 + (3*t^7.266)/g1^4 + 3*g1^8*t^7.468 + t^7.496/g1^30 + t^7.597/g1^24 + 2*g1^20*t^7.669 + t^7.698/g1^18 + t^7.798/g1^12 + g1^32*t^7.871 + t^7.899/g1^6 + t^8. + g1^6*t^8.101 + g1^12*t^8.202 + (2*t^8.23)/g1^26 + g1^24*t^8.403 + (2*t^8.431)/g1^14 + g1^30*t^8.504 - (2*t^8.532)/g1^8 + (2*t^8.633)/g1^2 + t^8.661/g1^40 - g1^4*t^8.734 + g1^48*t^8.806 + g1^10*t^8.835 + (2*t^8.863)/g1^28 - (g1^2*t^4.367)/y - (g1^14*t^6.569)/y + (g1^4*t^7.734)/y + (g1^16*t^7.935)/y + t^8.165/(g1^10*y) + t^8.266/(g1^4*y) + (g1^2*t^8.367)/y + (g1^8*t^8.468)/y + (g1^14*t^8.569)/y + (g1^20*t^8.669)/y + t^8.698/(g1^18*y) - (g1^26*t^8.77)/y + t^8.798/(g1^12*y) + (2*t^8.899)/(g1^6*y) - g1^2*t^4.367*y - g1^14*t^6.569*y + g1^4*t^7.734*y + g1^16*t^7.935*y + (t^8.165*y)/g1^10 + (t^8.266*y)/g1^4 + g1^2*t^8.367*y + g1^8*t^8.468*y + g1^14*t^8.569*y + g1^20*t^8.669*y + (t^8.698*y)/g1^18 - g1^26*t^8.77*y + (t^8.798*y)/g1^12 + (2*t^8.899*y)/g1^6 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1845 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6577 | 0.8161 | 0.8059 | [M:[1.1325, 1.1004, 0.9156, 0.8675, 0.6987], q:[0.7751, 0.3414], qb:[0.5262, 0.5582], phi:[0.4498]] | t^2.096 + t^2.603 + t^2.699 + t^2.747 + t^3.301 + t^3.349 + t^3.397 + t^3.952 + t^4. + t^4.048 + t^4.192 + t^4.506 + t^4.603 + 2*t^4.699 + t^4.795 + t^4.843 + t^5.205 + t^5.301 + 2*t^5.397 + t^5.446 + 2*t^5.494 + t^5.952 - t^6. - t^4.349/y - t^4.349*y | detail |