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 |
|---|---|---|---|---|---|---|---|---|---|
| 56888 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{1}M_{7}$ | 0.696 | 0.8549 | 0.8141 | [M:[1.0479, 0.9712, 0.9521, 1.0096, 1.0288, 0.9712, 0.9521], q:[0.5048, 0.4473], qb:[0.524, 0.5431], phi:[0.4952]] | [M:[[10], [-6], [-10], [2], [6], [-6], [-10]], q:[[1], [-11]], qb:[[5], [9]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{7}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}^{4}$ | ${}$ | -3 | 2*t^2.856 + 2*t^2.914 + t^2.971 + t^3.029 + t^3.201 + t^4.169 + t^4.342 + t^4.399 + t^4.457 + t^4.514 + t^4.572 + 2*t^4.629 + t^4.687 + t^4.744 + 2*t^5.712 + 3*t^5.77 + 4*t^5.827 + 3*t^5.885 + t^5.942 - 3*t^6. + t^6.115 - t^6.288 + t^6.403 + 2*t^7.025 + 2*t^7.083 + t^7.14 + t^7.198 + 2*t^7.256 + 3*t^7.313 + 4*t^7.371 + 2*t^7.428 + 2*t^7.486 + 3*t^7.543 + 4*t^7.601 + 2*t^7.658 - t^7.773 + t^7.831 + t^7.888 + t^7.946 + t^8.338 + t^8.511 + 3*t^8.569 + 3*t^8.626 + 5*t^8.684 + 7*t^8.741 + 5*t^8.799 - 2*t^8.856 - 5*t^8.914 - 4*t^8.971 - t^4.486/y - t^7.342/y - t^7.399/y + t^7.572/y + t^7.629/y + t^8.712/y + (4*t^8.77)/y + (3*t^8.827)/y + (4*t^8.885)/y + (2*t^8.942)/y - t^4.486*y - t^7.342*y - t^7.399*y + t^7.572*y + t^7.629*y + t^8.712*y + 4*t^8.77*y + 3*t^8.827*y + 4*t^8.885*y + 2*t^8.942*y | (2*t^2.856)/g1^10 + (2*t^2.914)/g1^6 + t^2.971/g1^2 + g1^2*t^3.029 + g1^14*t^3.201 + t^4.169/g1^23 + t^4.342/g1^11 + t^4.399/g1^7 + t^4.457/g1^3 + g1*t^4.514 + g1^5*t^4.572 + 2*g1^9*t^4.629 + g1^13*t^4.687 + g1^17*t^4.744 + (2*t^5.712)/g1^20 + (3*t^5.77)/g1^16 + (4*t^5.827)/g1^12 + (3*t^5.885)/g1^8 + t^5.942/g1^4 - 3*t^6. + g1^8*t^6.115 - g1^20*t^6.288 + g1^28*t^6.403 + (2*t^7.025)/g1^33 + (2*t^7.083)/g1^29 + t^7.14/g1^25 + t^7.198/g1^21 + (2*t^7.256)/g1^17 + (3*t^7.313)/g1^13 + (4*t^7.371)/g1^9 + (2*t^7.428)/g1^5 + (2*t^7.486)/g1 + 3*g1^3*t^7.543 + 4*g1^7*t^7.601 + 2*g1^11*t^7.658 - g1^19*t^7.773 + g1^23*t^7.831 + g1^27*t^7.888 + g1^31*t^7.946 + t^8.338/g1^46 + t^8.511/g1^34 + (3*t^8.569)/g1^30 + (3*t^8.626)/g1^26 + (5*t^8.684)/g1^22 + (7*t^8.741)/g1^18 + (5*t^8.799)/g1^14 - (2*t^8.856)/g1^10 - (5*t^8.914)/g1^6 - (4*t^8.971)/g1^2 - t^4.486/(g1*y) - t^7.342/(g1^11*y) - t^7.399/(g1^7*y) + (g1^5*t^7.572)/y + (g1^9*t^7.629)/y + t^8.712/(g1^20*y) + (4*t^8.77)/(g1^16*y) + (3*t^8.827)/(g1^12*y) + (4*t^8.885)/(g1^8*y) + (2*t^8.942)/(g1^4*y) - (t^4.486*y)/g1 - (t^7.342*y)/g1^11 - (t^7.399*y)/g1^7 + g1^5*t^7.572*y + g1^9*t^7.629*y + (t^8.712*y)/g1^20 + (4*t^8.77*y)/g1^16 + (3*t^8.827*y)/g1^12 + (4*t^8.885*y)/g1^8 + (2*t^8.942*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55248 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}M_{6}$ | 0.6926 | 0.8487 | 0.8161 | [M:[1.0247, 0.9852, 0.9753, 1.0049, 1.0148, 0.9852], q:[0.5025, 0.4729], qb:[0.5123, 0.5222], phi:[0.4975]] | t^2.926 + 2*t^2.956 + t^2.985 + t^3.015 + t^3.074 + t^3.104 + t^4.33 + t^4.419 + t^4.448 + t^4.478 + t^4.507 + t^4.537 + 2*t^4.567 + t^4.596 + t^4.626 + t^5.882 + 3*t^5.911 + 2*t^5.941 + t^5.97 - 2*t^6. - t^4.493/y - t^4.493*y | detail |