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 |
|---|---|---|---|---|---|---|---|---|---|
| 79545 | Sp2s2nf1 | ${}M_{1}S_{1}^{2}$ + ${ }M_{2}S_{2}^{2}$ + ${ }q_{2}^{2}S_{1}$ + ${ }M_{3}q_{1}q_{2}$ | 2.4157 | 2.5488 | 0.9478 | [X:[], M:[0.8714, 0.9028, 0.6776], q:[0.6045, 0.7178], qb:[], phi:[], S:[0.5643, 0.5486], Sb:[], A:[], Ab:[]] | [X:[], M:[[-4, 0], [0, -2], [12, 6]], q:[[-11, -6], [-1, 0]], qb:[], phi:[], S:[[2, 0], [0, 1]], Sb:[], A:[], Ab:[]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{1}$, ${ }M_{2}$, ${ }S_{1}S_{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{3}$, ${ }M_{1}^{2}$, ${ }q_{1}^{2}S_{2}$, ${ }q_{1}^{2}S_{1}$, ${ }M_{1}M_{2}$, ${ }M_{3}S_{1}S_{2}$, ${ }M_{2}^{2}$, ${ }q_{1}q_{2}S_{2}$, ${ }q_{2}^{2}S_{2}$ | ${}$ | -2 | t^2.033 + t^2.614 + t^2.708 + t^3.339 + t^4.066 + t^4.647 + t^4.741 + t^5.228 + t^5.273 + t^5.32 + t^5.322 + t^5.372 + t^5.417 + t^5.613 + t^5.953 - 2*t^6. + t^6.099 - t^6.34 + t^6.583 + t^6.63 + 3*t^6.678 + t^6.68 + t^6.725 + t^6.772 + t^6.774 + t^6.966 + t^7.259 + t^7.261 + 2*t^7.306 + t^7.353 + t^7.355 + t^7.405 + t^7.449 - t^7.693 + t^7.842 + t^7.887 + t^7.936 + t^8.029 + t^8.031 - 2*t^8.033 + t^8.125 + t^8.131 + t^8.227 - t^8.274 + t^8.565 + t^8.567 + 3*t^8.612 - 3*t^8.614 + t^8.616 + 3*t^8.659 + t^8.663 + t^8.706 - 2*t^8.708 + 3*t^8.71 + t^8.713 + t^8.758 + t^8.805 + t^8.807 + t^8.905 + 3*t^8.952 - t^8.954 + 2*t^8.999 - t^4.646/y - t^4.693/y - t^6.679/y - t^6.726/y - t^7.26/y - t^7.401/y + t^7.647/y + t^7.741/y - t^7.938/y - (2*t^7.985)/y - (2*t^8.032)/y - t^8.079/y + t^8.322/y + t^8.372/y - t^8.712/y - t^8.759/y + t^8.953/y - t^4.646*y - t^4.693*y - t^6.679*y - t^6.726*y - t^7.26*y - t^7.401*y + t^7.647*y + t^7.741*y - t^7.938*y - 2*t^7.985*y - 2*t^8.032*y - t^8.079*y + t^8.322*y + t^8.372*y - t^8.712*y - t^8.759*y + t^8.953*y | g1^12*g2^6*t^2.033 + t^2.614/g1^4 + t^2.708/g2^2 + g1^2*g2*t^3.339 + g1^24*g2^12*t^4.066 + g1^8*g2^6*t^4.647 + g1^12*g2^4*t^4.741 + t^5.228/g1^8 + t^5.273/(g1^22*g2^11) + t^5.32/(g1^20*g2^12) + t^5.322/(g1^4*g2^2) + g1^14*g2^7*t^5.372 + t^5.417/g2^4 + t^5.613/(g1^12*g2^5) + (g2*t^5.953)/g1^2 - 2*t^6. + g1^36*g2^18*t^6.099 - g1^10*g2^6*t^6.34 + g2^4*t^6.583 + g1^2*g2^3*t^6.63 + 3*g1^4*g2^2*t^6.678 + g1^20*g2^12*t^6.68 + g1^6*g2*t^6.725 + g1^8*t^6.772 + g1^24*g2^10*t^6.774 + t^6.966/(g1^20*g2^11) + t^7.259/(g1^12*g2^4) + g1^4*g2^6*t^7.261 + (2*t^7.306)/(g1^10*g2^5) + t^7.353/(g1^8*g2^6) + g1^8*g2^4*t^7.355 + g1^26*g2^13*t^7.405 + g1^12*g2^2*t^7.449 - g1^2*t^7.693 + t^7.842/g1^12 + t^7.887/(g1^26*g2^11) + t^7.936/(g1^8*g2^2) + t^8.029/(g1^20*g2^14) + t^8.031/(g1^4*g2^4) - 2*g1^12*g2^6*t^8.033 + t^8.125/g2^6 + g1^48*g2^24*t^8.131 + t^8.227/(g1^16*g2^5) - t^8.274/(g1^14*g2^6) + t^8.565/(g1^22*g2^9) + (g2*t^8.567)/g1^6 + (3*t^8.612)/(g1^20*g2^10) - (3*t^8.614)/g1^4 + g1^12*g2^10*t^8.616 + (3*t^8.659)/(g1^18*g2^11) + g1^14*g2^9*t^8.663 + t^8.706/(g1^16*g2^12) - (2*t^8.708)/g2^2 + 3*g1^16*g2^8*t^8.71 + g1^32*g2^18*t^8.713 + g1^18*g2^7*t^8.758 + g1^20*g2^6*t^8.805 + g1^36*g2^16*t^8.807 + t^8.905/(g1^12*g2^3) + (3*t^8.952)/(g1^10*g2^4) - g1^6*g2^6*t^8.954 + (2*t^8.999)/(g1^8*g2^5) - (g2*t^4.646)/y - (g1^2*t^4.693)/y - (g1^12*g2^7*t^6.679)/y - (g1^14*g2^6*t^6.726)/y - (g2*t^7.26)/(g1^4*y) - (g1^2*t^7.401)/(g2^2*y) + (g1^8*g2^6*t^7.647)/y + (g1^12*g2^4*t^7.741)/y - (g2^3*t^7.938)/y - (2*g1^2*g2^2*t^7.985)/y - (2*g1^4*g2*t^8.032)/y - (g1^6*t^8.079)/y + t^8.322/(g1^4*g2^2*y) + (g1^14*g2^7*t^8.372)/y - (g1^24*g2^13*t^8.712)/y - (g1^26*g2^12*t^8.759)/y + (g2*t^8.953)/(g1^2*y) - g2*t^4.646*y - g1^2*t^4.693*y - g1^12*g2^7*t^6.679*y - g1^14*g2^6*t^6.726*y - (g2*t^7.26*y)/g1^4 - (g1^2*t^7.401*y)/g2^2 + g1^8*g2^6*t^7.647*y + g1^12*g2^4*t^7.741*y - g2^3*t^7.938*y - 2*g1^2*g2^2*t^7.985*y - 2*g1^4*g2*t^8.032*y - g1^6*t^8.079*y + (t^8.322*y)/(g1^4*g2^2) + g1^14*g2^7*t^8.372*y - g1^24*g2^13*t^8.712*y - g1^26*g2^12*t^8.759*y + (g2*t^8.953*y)/g1^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 79519 | Sp2s2nf1 | ${}M_{1}S_{1}^{2}$ + ${ }M_{2}S_{2}^{2}$ + ${ }q_{2}^{2}S_{1}$ | 2.395 | 2.5083 | 0.9548 | [X:[], M:[0.8706, 0.9027], q:[0.6023, 0.7177], qb:[], phi:[], S:[0.5647, 0.5486], Sb:[], A:[], Ab:[]] | t^2.612 + t^2.708 + t^3.34 + t^3.96 + t^5.224 + t^5.26 + t^5.308 + t^5.32 + t^5.416 + t^5.606 + t^5.952 - 2*t^6. - t^4.646/y - t^4.694/y - t^4.646*y - t^4.694*y | detail |