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 |
|---|---|---|---|---|---|---|---|---|---|
| 2533 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{5}M_{7}$ | 0.6993 | 0.8588 | 0.8143 | [M:[1.0, 0.9582, 1.0209, 0.9372, 1.0628, 0.9791, 0.9372], q:[0.5209, 0.4791], qb:[0.4582, 0.5837], phi:[0.4895]] | [M:[[0], [-4], [2], [-6], [6], [-2], [-6]], q:[[2], [-2]], qb:[[-4], [8]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{7}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{7}$, ${ }M_{2}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$ | ${}$ | -3 | 2*t^2.812 + t^2.874 + 2*t^2.937 + t^3. + t^3.314 + t^4.218 + t^4.28 + t^4.343 + t^4.406 + t^4.469 + 2*t^4.594 + t^4.657 + t^4.782 + t^4.971 + 2*t^5.623 + t^5.686 + 5*t^5.749 + 2*t^5.812 + 3*t^5.874 + t^5.937 - 3*t^6. - t^6.063 - t^6.188 + 2*t^6.251 - t^6.377 + t^6.628 + 2*t^7.029 + 2*t^7.092 + 4*t^7.155 + 5*t^7.218 + 2*t^7.28 + 2*t^7.343 + 3*t^7.406 + 3*t^7.531 + 3*t^7.594 - 2*t^7.657 + t^7.72 + t^7.782 - t^7.845 + 3*t^7.908 + t^7.971 - t^8.034 + t^8.096 + t^8.285 + 3*t^8.435 + 2*t^8.498 + 6*t^8.561 + 4*t^8.623 + 8*t^8.686 + 2*t^8.749 - t^8.874 - 7*t^8.937 - t^4.469/y - t^7.28/y - t^7.343/y - t^7.406/y + t^7.531/y + t^7.594/y + t^7.657/y + t^8.623/y + (2*t^8.686)/y + (4*t^8.749)/y + (4*t^8.812)/y + (2*t^8.874)/y + (2*t^8.937)/y - t^4.469*y - t^7.28*y - t^7.343*y - t^7.406*y + t^7.531*y + t^7.594*y + t^7.657*y + t^8.623*y + 2*t^8.686*y + 4*t^8.749*y + 4*t^8.812*y + 2*t^8.874*y + 2*t^8.937*y | (2*t^2.812)/g1^6 + t^2.874/g1^4 + (2*t^2.937)/g1^2 + t^3. + g1^10*t^3.314 + t^4.218/g1^9 + t^4.28/g1^7 + t^4.343/g1^5 + t^4.406/g1^3 + t^4.469/g1 + 2*g1^3*t^4.594 + g1^5*t^4.657 + g1^9*t^4.782 + g1^15*t^4.971 + (2*t^5.623)/g1^12 + t^5.686/g1^10 + (5*t^5.749)/g1^8 + (2*t^5.812)/g1^6 + (3*t^5.874)/g1^4 + t^5.937/g1^2 - 3*t^6. - g1^2*t^6.063 - g1^6*t^6.188 + 2*g1^8*t^6.251 - g1^12*t^6.377 + g1^20*t^6.628 + (2*t^7.029)/g1^15 + (2*t^7.092)/g1^13 + (4*t^7.155)/g1^11 + (5*t^7.218)/g1^9 + (2*t^7.28)/g1^7 + (2*t^7.343)/g1^5 + (3*t^7.406)/g1^3 + 3*g1*t^7.531 + 3*g1^3*t^7.594 - 2*g1^5*t^7.657 + g1^7*t^7.72 + g1^9*t^7.782 - g1^11*t^7.845 + 3*g1^13*t^7.908 + g1^15*t^7.971 - g1^17*t^8.034 + g1^19*t^8.096 + g1^25*t^8.285 + (3*t^8.435)/g1^18 + (2*t^8.498)/g1^16 + (6*t^8.561)/g1^14 + (4*t^8.623)/g1^12 + (8*t^8.686)/g1^10 + (2*t^8.749)/g1^8 - t^8.874/g1^4 - (7*t^8.937)/g1^2 - t^4.469/(g1*y) - t^7.28/(g1^7*y) - t^7.343/(g1^5*y) - t^7.406/(g1^3*y) + (g1*t^7.531)/y + (g1^3*t^7.594)/y + (g1^5*t^7.657)/y + t^8.623/(g1^12*y) + (2*t^8.686)/(g1^10*y) + (4*t^8.749)/(g1^8*y) + (4*t^8.812)/(g1^6*y) + (2*t^8.874)/(g1^4*y) + (2*t^8.937)/(g1^2*y) - (t^4.469*y)/g1 - (t^7.28*y)/g1^7 - (t^7.343*y)/g1^5 - (t^7.406*y)/g1^3 + g1*t^7.531*y + g1^3*t^7.594*y + g1^5*t^7.657*y + (t^8.623*y)/g1^12 + (2*t^8.686*y)/g1^10 + (4*t^8.749*y)/g1^8 + (4*t^8.812*y)/g1^6 + (2*t^8.874*y)/g1^4 + (2*t^8.937*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1457 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ | 0.6945 | 0.8504 | 0.8167 | [M:[1.0, 0.9738, 1.0131, 0.9606, 1.0394, 0.9869], q:[0.5131, 0.4869], qb:[0.4738, 0.5525], phi:[0.4934]] | t^2.882 + t^2.921 + 2*t^2.961 + t^3. + t^3.118 + t^3.197 + t^4.323 + t^4.362 + t^4.402 + t^4.441 + t^4.48 + 2*t^4.559 + t^4.598 + t^4.677 + t^4.795 + 3*t^5.843 + t^5.882 + 3*t^5.921 + t^5.961 - 2*t^6. - t^4.48/y - t^4.48*y | detail |