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 |
|---|---|---|---|---|---|---|---|---|---|
| 2602 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{5}M_{6}$ + ${ }M_{3}M_{7}$ | 0.7056 | 0.8691 | 0.8119 | [M:[1.0, 0.9336, 1.0664, 0.8672, 1.0332, 0.9668, 0.9336], q:[0.4834, 0.5166], qb:[0.4502, 0.6162], phi:[0.4834]] | [M:[[0], [-4], [4], [-8], [2], [-2], [-4]], q:[[-1], [1]], qb:[[-3], [7]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{2}$, ${ }M_{7}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$ | ${}$ | -3 | t^2.601 + 2*t^2.801 + 2*t^2.9 + t^3. + t^3.299 + t^4.151 + t^4.251 + 2*t^4.351 + t^4.45 + t^4.55 + t^4.649 + t^4.749 + t^4.849 + t^5.148 + t^5.203 + 2*t^5.402 + t^5.502 + 3*t^5.601 + 3*t^5.701 + 4*t^5.801 + t^5.9 - 3*t^6. - t^6.399 - t^6.498 + t^6.598 + t^6.753 + t^6.852 + 3*t^6.952 + 4*t^7.052 + 6*t^7.151 + 5*t^7.251 + 3*t^7.351 + t^7.45 + t^7.55 + 2*t^7.649 + t^7.749 + t^7.804 - t^7.849 + 2*t^8.004 + 2*t^8.048 + t^8.103 + t^8.148 + 3*t^8.203 - t^8.247 + 3*t^8.303 + 5*t^8.402 + t^8.446 + 5*t^8.502 + 4*t^8.601 + 5*t^8.701 - 4*t^8.801 - 5*t^8.9 - t^4.45/y - t^7.052/y - t^7.251/y - t^7.351/y + t^7.55/y + t^7.649/y + t^7.849/y + (2*t^8.402)/y + (2*t^8.502)/y + (2*t^8.601)/y + (4*t^8.701)/y + (3*t^8.801)/y + (3*t^8.9)/y - t^4.45*y - t^7.052*y - t^7.251*y - t^7.351*y + t^7.55*y + t^7.649*y + t^7.849*y + 2*t^8.402*y + 2*t^8.502*y + 2*t^8.601*y + 4*t^8.701*y + 3*t^8.801*y + 3*t^8.9*y | t^2.601/g1^8 + (2*t^2.801)/g1^4 + (2*t^2.9)/g1^2 + t^3. + g1^6*t^3.299 + t^4.151/g1^7 + t^4.251/g1^5 + (2*t^4.351)/g1^3 + t^4.45/g1 + g1*t^4.55 + g1^3*t^4.649 + g1^5*t^4.749 + g1^7*t^4.849 + g1^13*t^5.148 + t^5.203/g1^16 + (2*t^5.402)/g1^12 + t^5.502/g1^10 + (3*t^5.601)/g1^8 + (3*t^5.701)/g1^6 + (4*t^5.801)/g1^4 + t^5.9/g1^2 - 3*t^6. - g1^8*t^6.399 - g1^10*t^6.498 + g1^12*t^6.598 + t^6.753/g1^15 + t^6.852/g1^13 + (3*t^6.952)/g1^11 + (4*t^7.052)/g1^9 + (6*t^7.151)/g1^7 + (5*t^7.251)/g1^5 + (3*t^7.351)/g1^3 + t^7.45/g1 + g1*t^7.55 + 2*g1^3*t^7.649 + g1^5*t^7.749 + t^7.804/g1^24 - g1^7*t^7.849 + (2*t^8.004)/g1^20 + 2*g1^11*t^8.048 + t^8.103/g1^18 + g1^13*t^8.148 + (3*t^8.203)/g1^16 - g1^15*t^8.247 + (3*t^8.303)/g1^14 + (5*t^8.402)/g1^12 + g1^19*t^8.446 + (5*t^8.502)/g1^10 + (4*t^8.601)/g1^8 + (5*t^8.701)/g1^6 - (4*t^8.801)/g1^4 - (5*t^8.9)/g1^2 - t^4.45/(g1*y) - t^7.052/(g1^9*y) - t^7.251/(g1^5*y) - t^7.351/(g1^3*y) + (g1*t^7.55)/y + (g1^3*t^7.649)/y + (g1^7*t^7.849)/y + (2*t^8.402)/(g1^12*y) + (2*t^8.502)/(g1^10*y) + (2*t^8.601)/(g1^8*y) + (4*t^8.701)/(g1^6*y) + (3*t^8.801)/(g1^4*y) + (3*t^8.9)/(g1^2*y) - (t^4.45*y)/g1 - (t^7.052*y)/g1^9 - (t^7.251*y)/g1^5 - (t^7.351*y)/g1^3 + g1*t^7.55*y + g1^3*t^7.649*y + g1^7*t^7.849*y + (2*t^8.402*y)/g1^12 + (2*t^8.502*y)/g1^10 + (2*t^8.601*y)/g1^8 + (4*t^8.701*y)/g1^6 + (3*t^8.801*y)/g1^4 + (3*t^8.9*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1507 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{5}M_{6}$ | 0.7001 | 0.8588 | 0.8152 | [M:[1.0, 0.9479, 1.0521, 0.8957, 1.0261, 0.9739], q:[0.487, 0.513], qb:[0.4609, 0.5912], phi:[0.487]] | t^2.687 + t^2.844 + 2*t^2.922 + t^3. + t^3.156 + t^3.235 + t^4.226 + t^4.304 + 2*t^4.383 + t^4.461 + t^4.539 + t^4.617 + t^4.696 + t^4.774 + t^5.008 + t^5.374 + t^5.531 + t^5.609 + t^5.687 + t^5.765 + 4*t^5.844 + t^5.922 - 2*t^6. - t^4.461/y - t^4.461*y | detail |